Building material

专利摘要:
The present invention relates to a building material (110) comprising at least one conductive low-emissivity surface (103) provided with an opening (203) for intensifying transmission of an electromagnetic signal through a building material, and wherein the opening has a substantially less electrical conductivity than the low-emissivity surface ( 103). The edge of said aperture (203) provided in the low-emissivity surface (103) forms at least one closed edge curve (223), and said aperture (203) defines a closed envelope curve (224) such that said aperture (203) lies within the closed envelope curve (224) , and wherein the area bounded by the closed envelope curve (224) has a surface substantially larger than the surface of the opening (203) within the closed envelope curve (224), and a length substantially less than the length of the closed edge curve (223), at least an area (231) of the low emissivity surface (103) is formed within the area defined by the closed envelope curve (224) at which the closed envelope curve (224) does not coincide with the edge curve (223). Said conductive region (231) on the low emissivity surface (103) defines at least two edges of the aperture (203), which are arranged at at least one distance (234), and wherein said edges are at least partially wrap-around.
公开号:FI20185840A1
申请号:FI20185840
申请日:2018-01-11
公开日:2019-04-11
发明作者:Juha Lilja
申请人:Stealthcase Oy；
IPC主号:

专利说明:

building Supplies
Object of the invention
The present invention relates to a building material comprising at least an electrically conductive low-ejection surface having a radio-transmitting aperture for enhancing the transmission of an electromagnetic signal. The invention further relates to a method for manufacturing an insulating glass element, and to a method for transmitting radio signals from one side to the other side of an insulating glass element 10.
Background of the Invention
The construction industry's ambitions for passive and zero energy houses have led to a situation where high-performance thermal insulation strongly suppresses signals from cellular phones and other wireless systems, which can make it even impossible to use a cellphone inside the building. There are many reasons for this suppression, but one of the causes is the so-called. use of selective glasses, where the windows are coated with electrically conductive coatings 20 with low coverage coatings.
Communication between wireless communication devices, such as mobile phones, tablets, or sensors classified as Internet of Things (IOT), is based on the management of electromagnetic energy, that is to say the ability to receive and read electromagnetic waves, and the information associated with them. Controlled combining of information into a portion of an electromagnetic wave is called modulation, while controlled decompression of this information from an electromagnetic wave is called demodulation. An individual discrete sinusoidal oscillating frequency component which is part of an electromagnetic spectrum can be called an electromagnetic signal. Alternatively, in some contexts, an electromagnetic signal may also be referred to as a portion of the electromagnetic spectrum having
20185840 prh 08 -10-2018 The combination of discrete frequency components contained in the propagating electromagnetic energy bears some of the information transmitted.
Most of the electromagnetic spectrum bands currently in use in mobile phones are classified in the UHF frequency band (300 MHz to 3GHz) and, to an increasing extent, also in the SHF frequencies (3-30 GHz). Frequency allocations for new short-range mobile communications are also planned in the EHF range (30-300 GHz).
Wireless communication can be either one-way or two-way. For conventional mobile devices, communication with base stations is bidirectional, whereas communication with wireless sensors, for example, can be unidirectional. Operation of such a wireless communication connection is required when the sensitivity level of the device receiving the sig15 wireless signal is sufficiently low in relation to the power level of the received signal. A significant factor affecting the sensitivity of the receiving device is the noise level generated by the device's own electronic circuits; signals with lower power levels than noise are difficult to receive without losing some of the signal information. Also, the addition of electromagnetic interference from the receiver environment to the received signal may reduce the quality of the communication connection and cause connection problems.
The power level of the received signal is influenced, for example, by adjusting the transmission power of the transmitting device and, in the case of mobile networks, by designing a base station communication network sufficiently dense. However, building attenuation, which is a significant disadvantage to this communication link, is a particularly challenging problem because it significantly weakens the functionality of wireless communication links across building walls. In typical low energy buildings, the attenuations measured may be, for example, values between 20 and 50 dB. By way of comparison, each six decibel (6 dB) power increase in transmit power on average doubles the link spacing in free space. Conversely, each additional six decibel attenuation on average halves the maximum theoretical link 35. Building cushioning is thus a major disadvantage to the wireless links brought
20185840 prh 08 -10-2018 design distances, and for practical reasons it cannot be compensated by a mere increase in transmission power. In addition, at least one device in the communication interval, such as a cellular telephone, is most often a battery-powered device, which always aims to minimize the transmission power in order to maximize battery life.
Conventionally, signals from wireless systems can enter through windows in buildings, but electrically conductive low-activity coatings block these signal paths. In addition to windows, electromagnetic signals have previously been able to penetrate the walls of buildings, but 10 aluminum-coated thermal insulation panels, which are now commonly used in walls, effectively prevent signals from entering the building. Also, reinforcements in concrete structures, together with electronically high loss cement, can dampen electromagnetic signals, whereby, even when passing through such a structure, the signal strength may be too weak to have, for example, a signal strength sufficient to operate a mobile phone.
Attempts have been made to solve this problem, for example, by a passive antenna system comprising two separate antennas and a transmission line 20 connecting the two antennas. However, the challenge of a passive antenna repeater is that, in order to operate at an even level, it must be precisely directed towards the operator's base station.
Other solutions are also known, such as frequency-selective surfaces (Frequency 25 Selective Surface (FSS)), in which periodic lattice structures are formed over a wide area of the glass to reduce the permeability of the glass. The frequency-selective surfaces formed on the surface of the glasses are planar, two-dimensional filters that can be designed as either band-stop, band-pass, high-pass, or low-pass filters. Frequency selective30 surfaces are generally well known also in the art of screened glass. For example, in U.S. Patent No. 5,364,685 A to Central Glass Company, periodic discontinuous portions, such as incision-like slits or lattice-shaped FSS filters, are formed on a laminated selective glass to improve transmission of the electromagnetic signal. Also in US 6,730,389 35 B2 FSS filters are formed on the surface of a selective film for the same problem.
20185840 prh 08 -10- 2018 to resolve this issue. Typically, the topologies used in the elements of the FSS filter are various loops, as in US 8,633,866 B2.
US 6356236 B1 also discloses a frequency-selective surface arranged on a low-emissivity surface, wherein said surface comprises a lattice-frequency-selective region, and wherein said low-emissivity surface is laminated between two glasses.
For frequency-selective surfaces formed on glass surfaces, the first technical problem is the large processing area they require. The coating can be removed by, for example, laser, etching, or mechanical machining. The coating removal device shall be capable of processing the selective surface both in the width direction and in the longitudinal direction of the glass. In continuous mass production, this is technically difficult to accomplish with the precision and speed required by process 15. The frequency-selective surface, which encompasses a wide processing industry, is also a delicate eye-quality defect in the window glass.
The frequency-selective surfaces formed on the glass surface also have another technical problem due to the low electrical conductivity of the selective surface. Frequency-selective surfaces made on the surface of typical metals such as aluminum or copper can achieve very low transmittance damping on the electromagnetic signal. However, the frequency-selective surface provided on the selective surface of the glass has significantly higher resistive losses, which is reflected in a decrease in the permeation efficiency. For example, the surface resistances of low-emissivity surfaces used on glass surfaces may be in the range of 10-100 Ω / square, though in some cases also somewhat less and in some cases much more. The wide range of surface resistances is due to the wide application of coatings. Some of the low-cut side 30 coatings are used in the gas-insulated space of the thermal glazing element, while some are used on the outer layers of the glazing or laminated between the two glass panes. In a generally gas-insulated space, so-called. soft film, while the outer glass surfaces use so-called "soft" film. hard film mm. to eliminate the strain on the window caused by outdoor air and cleaning.
Coatings on the outermost glass surfaces can influence, for example, light transmission, solar energy filtering, or fogging of the glasses.
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The frequency-selective surfaces formed on the glass surface also have a third technical problem due to the effect of increasing the size of the transmitting aperture on the summing of the transmitting waves. In practice, this is reflected by the fact that the reflection pattern formed by the surface, which can also be depicted antenna-directionally, is usually determined by a narrow beam in a single maximum direction, where the orientation of the maximum direction is determined by the direction of the incoming electromagnetic wave. The frequency-selective surface penetration characteristics typically decrease when the electromagnetic signal illuminating the surface arrives from a direction other than the primary maximum. In other words, if the permeability properties of the surface are optimized, for example, for an electromagnetic signal coming from the normal direction of the glass surface, due to its symmetry the direction pattern of the electromagnetic wave passing through it is concentrated inside the relatively narrow beam. This is not a favorable feature for improving the weather coverage of the mobile network si15 because the location of the base stations and the location of the wireless device are both unknown and unpredictable. In practice, penetration can be effective only in individual cases where both the base station's outdoor location and the wireless device's location inside the building are in carefully selected directions.
One technical problem is related to the dependence between the open areas of the low-surface area of the building material and the heat insulation capacity. For example, in Utility Model Application U20144180 - StealthCase Oy, it is stated that one or more electrically conductive surfaces of a glass can be made with 25 non-conducting points (openings), i.e., not coated at points intended to form fracture radiators. discontinuities, and which may advantageously have an elongated shape. For example, a wide band gap radiator can be implemented with a wide aperture 30 whose resonance impedance can be matched to the wave impedance of an electromagnetic wave propagating through the air, but the wide aperture surface forms a thermal energy leakage region if implemented at a low emptying surface. In addition to reflecting the wave due to the impedance of a single narrow opening, the performance of a single narrow opening is also impaired by the behavior of currents around the opening. With a narrow opening, the actual electromagnetic radiation is the current mode
20185840 prh 08 -10-2018, the current generating remains relatively low, while the narrow-open reciprocal current is too high. The two equally hateful currents of almost equal magnitude in opposite directions cancel out the radiation from each other. A solution to increase heat loss would be to widen the aperture, thereby making the behavior of the currents more favorable to the generation of radiation. A solution according to a preferred embodiment of the present invention cancels out said reverse radiation attenuating currents, thereby making narrow openings more efficient radiators.
The planar frequency-selective surface formed on the selective surface on the glass surface has similar technical properties to a large light aperture without a selective film. In practice, this means that the diffraction of the electromagnetic wave from the 15 apertures in question behaves in the same way as a wide aperture, where the aperture width is several wavelengths. The diffraction pattern caused by the wide aperture differs significantly from the diffraction pattern of the narrow aperture.
Minimizing wireless signal attenuation is often the primary means of improving the quality of the connection, or even creating the conditions for wireless connection in the dark. Modern wireless communication systems are also capable of increasing the quality of wireless communication over multiple parallel communication channels, in which parallel channels are established on physically unrelated propagation channels. This approach has already become an almost indispensable part of modern systems, such as those used in 3G and 4G network diversity technologies, as well as 4G and future 5G (IMT-2020) networks ΜΙΜΟ (Multiple Input) and Massive MIMO- techniques.
MIMO techniques are based on uncorrelated data streams created by multiple transmitter and receiver antennas. Techniques can be used to improve connectivity problems due to multipath propagation (diversity gain), or to increase the capacity and spectral efficiency of the wireless communication channel, thereby increasing the maximum data transfer rate to be achieved within a specified time.
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Wireless transmission itself is an environment that is constantly changing in time and place and is very damaging to the wireless signal. However, multipath propagation can be utilized to make the connection more efficient. The starting point for exploiting diversity and MIMO techniques is the rich scattering environment.
Multipath components are always present, but there are major differences between scattering environments. In buildings, one of the major structural challenges to the scattering environment is the very limited signal direction. Conventionally, the outer envelope of a building is capable of receiving substantially more multi-path10 signal components than the internal structures of a building, which dampen signals from almost any open aperture.
One way to improve the scattering environment inside a building is to ensure that the base station network outside the building is scattered indoors from multiple locations and directions. Multiple directions mean not only the use of multiple apertures in the wall structure of a single room, but also the consideration of multiple directions of entry outside the mantle.
Another way to enhance the indoor scattering environment of a building is to ensure that more signals arriving in non-correlated polarizations are scattered across the building's room.
A rich scattering environment inside buildings, based on an external access point network, is a particularly effective way to improve the quality of indoor communication. Diversity-based wireless communication devices are capable of operating at lower signal strengths than wireless diversity-free wireless devices if correlated 30 towers of signal currents are brought inside a building.
BRIEF SUMMARY OF THE INVENTION
It is an object of the present invention to provide an improved building material 35 in which the aforementioned drawbacks are substantially eliminated. Now
20185840 prh 08 -10-2018 the present invention is based on the idea that the edge of said opening on the low side surface forms at least one closed edge curve, and that the edge of said opening on the low side surface forms at least one closed edge curve, and that said opening 5 defines a closed curtain the aperture is within the closed curve and the area of the area enclosed by the closed curve is substantially larger than the area and length of the inner opening of the closed curve substantially less than the length of the closed periphery, thereby forming at least one the closed envelope does not coincide with the edge curve.
In addition to solving the above technical problems, one of the advantageous features of the present invention is the optimization of the gap radiator impedance matching 15 and the bandwidth so that the physical area of the electrically non-conducting region formed on the low emitting surface can be miniaturized.
It is well known in the art of conventional coaxial cable or planar transmission line such as microstrip 20 or coplanar wire how the gap width affects the impedance of the slot antenna. According to the Babinet principle, an impedance equivalent to the impedance of a dipole antenna can be calculated for the gap antenna impedance. It is known from dipole antennas how the widening of the antenna's wires widen the antenna's operating bandwidth, for example using a conventional 50 Ω transmission line as the input impedance. Correspondingly, the impedance behavior of the slit antenna fed by the transmission line as a function of frequency is favored against this impedance when the slit antenna slit width can be widened.
A similar analogy can also be found with a resonant opening formed on an electrically conductive coating, where an electric field vector comprising a non-conductive region of the opening forms a resonant circuit with a surface current oscillating in the conductive region delimited by the edge. The impedance of the opening is determined by the ratio of the electric field to the magnetic field 35. In a typical case, for example a rectangle
20185840 prh 08 -10-2018 Broadband adaptation of the impedance of a tea-shaped resonant aperture to a free-space wave impedance occurs, for example, with 20-40 mm wide apertures, although this strongly depends on the properties of the dielectric material, for example.
The purpose of the low-level surface is to reduce the amount of thermal radiation that penetrates the building envelope. The implementation of wide openings such as the preceding example on a low-emitting surface causes local weakening of the thermal radiation insulation capacity. Similarly, with narrow single apertures 10 without the use of parallel resonances, such as
At 100 µm wide openings, achieving wide impedance matching with low emitting surface gap radiators is challenging.
It is an object of a preferred embodiment of the present invention to solve the above problem by substantially reducing the physical surface area of the aperture formed on the low-emptying surface while achieving a behavior favorable to the aperture matching of the aperture, wherein the impedance of the aperture according to their behavior. A low aperture formed by a curving narrow linear aperture is formed on the low activity surface, the silhouette of which defines an area substantially larger than the physical area of the aperture.
One advantage of the curving edge curve of a narrow linear opening is also the extension of the path of the resonating current loop. This means that the physical surface area required by the antenna is reduced compared to a similar opening tuned to the same frequency range, which does not utilize the curved opening edge curve presented herein.
Specifically, the building element of the present invention is essentially characterized by what is set forth in the characterizing part of claim 1 of the appended claims. The method according to the present invention is essentially characterized by what is set forth in the characterizing part of the appended claim 35.
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The present invention enhances the passage of an electromagnetic signal through an electrically conductive low emitting surface based on narrow aperture diffraction, whereby a broader electromagnetic wave coverage than a wide aper5 diffraction solution can be applied to the interior of the building.
Some preferred embodiments of the present invention compensate for low efficiency conductivity surface losses typically caused by low conductivity low surface area losses by arranging differential currents to form low emissivity surface opening portions so that the radiation efficiency partially decreases the current efficiency.
In addition, the present invention compensates for the weakening of efficiency typically caused by low conductivity low surface conductivity surface loss by increasing the signal transmission efficiency on a coherent wavefront formed by a plurality of focused gap radiators.
The present invention enhances the passage of an electromagnetic signal through an electrically conductive low-emitting surface by creating a virtual aperture formed by low-emitting surface radiation sources having an effective electromagnetic energy-receiving surface greater than that created by the low-emitting surface.
The present invention further enhances the passage of an electromagnetic signal through an electrically conductive low-emitting surface based on narrow aperture diffraction, whereby, using known solutions indoors, a wider electromagnetic wave coverage than a wide aperture diffraction can be introduced into the blind spot.
The operation of the device of the present invention is based on the re-irradiation of the electric35 magnetic energy received from the electromagnetic planar surface in a low emitted surface with a plurality of concentrated wave sources11.
20185840 prh 08 -10-2018, wherein a portion of the electromagnetic wave received from the planar wave is redirected to the opposite side of the low-emitting surface surface by utilizing constructive interference. Coherent transmission from multiple mutually reinforcing focused radiation sources compensates for the loss of efficiency due to resistive conductor surface losses.
The operation of the device according to the present invention is further based on the operation of slit radiators formed on a low-emitting surface as point-centered radiation sources, where preferably a coherent wavefront formed by slit radiators located below the wavelength of operation is summed in the desired gain direction. A preferred utility direction for the slit radiator array formed with the insulating glass element is a horizontal plane in which the wavefront formed by the slit radiator 15 group forms a flat directional pattern. In the horizontal plane, the maximum wide directional pattern outside the insulating glass and the interior effectively receives the base station signal from the horizon, and creates a wide indoor coverage relative to the insulating glass element of the wall-mounted window in the horizontal plane.
A locally concentrated radiation source is visible as a point source radiation when viewed in its far field by an electromagnetic wave emitted by it. For example, the wavelength, half wavelength, or scale, for example, a quarter-wave radiation source is seen to be a point source of radiation 25 as the emitted wave front looking at a sufficient distance, in other words, the far field.
It is an object of the present invention to enhance the quality and capacity of wireless communication connections based on an external base station network used in buildings by increasing the number of uncorrelated communication channels that pass through the building envelope. The device of the present invention improves the scattering environment inside a building by receiving two electromagnetic signals arriving in cross polarization from the building envelope, and retransmitting these 35 electromagnetic signals received in cross polarization into the interior of the building.
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An embodiment of a preferred embodiment of the present invention comprises two cross-polarized apertures transmitting a radio signal, which further comprise cross-polarized concentrated radiation sources to re-radiate the electric energy of the building material electromagnetic signal.
An embodiment of a preferred embodiment of the present invention comprises two circularly polarized radio-transmissive apertures in which the directions of rotation of the polarizations are transverse.
An embodiment of a preferred embodiment of the present invention comprises a load impedance arranged in connection with a low-emitting surface and a control unit which can be used to control the radiation pattern formed by the Building Material. Said radiation pattern control can be used, for example, to improve wireless connections to base stations, filter interference signals, or optimize wireless network resourcing.
Description of the drawings
The present invention will now be described in more detail with reference to the accompanying drawings in which
Fig. 1a shows a construction material according to a preferred embodiment of the present invention,
Figure 1b shows a detail of the Building Material in Figure 1a,
Figures 2a-2d show an insulating glass element comprising at least two glass sheets, with an intermediate space between them, at least one of which is provided with said low edge surface,
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Figures 3a and 3b illustrate an example of a coherent wavefront caused by a plurality of concentrated radiation sources comprising a narrow aperture,
Figure 3c shows a detail of the slit radiator of Figure 3b,
Figure 4 illustrates, in accordance with a preferred embodiment of the present invention, a gap radiator array arranged in a building surface comprising a low-cut line 10 on a building surface,
Figures 5a-5c illustrate examples of openings according to some preferred embodiments of the present invention in the lowering side 15,
Figures 6a-6c show examples of openings in a low-relief web surface according to some preferred embodiments of the present invention,
Figures 7a-7c illustrate slit radiators of a ra 25 radiator array comprising a radio transmitting aperture according to a preferred embodiment of the present invention arranged in connection with a lattice structure.
Figures 8a-8c show arrangements for opening low-level surface openings in accordance with certain preferred embodiments of the present invention30 for canceling differential current jets,
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Figures 9a and 9b show longitudinally distributed components arranged in a low-emptying surface according to a preferred embodiment of the present invention for arranging an opening load impedance,
Figures 10a-10d illustrate examples of implementing load impedances according to some preferred embodiments of the present invention, and
Figures 11a-11e illustrate examples of embodiments according to some preferred embodiments of the present invention for adjusting the transmission characteristics of a low-pass aperture comprising a radio signal.
Detailed Description of the Invention
Fig. 1a illustrates a typical building material 110 comprising an electrically conductive low-emissivity surface 103. Provided to enhance the thermal insulation properties of the building material. or aluminum-plastic composites for facades.
Fig. 1a illustrates an arrangement according to a preferred embodiment of the present invention, wherein the building material 110 comprises at least one electrically conductive low-emptying surface 103 provided with an opening
203 to enhance the passage of the electromagnetic signal through the Building Material, and the opening of which has a substantially lower electrical conductivity than the low emptying surface 103.
Fig. 1b illustrates in more detail the opening 203 in Fig. 1a, with the edge of said opening 203 arranged on the low-side surface 103
20185840 prh 08 -10-2018 forms at least one closed edge curve 223, and said opening 203 defines a closed envelope 224 such that said opening 203 is inside the closed envelope 224 and has a surface area substantially delimited by the closed envelope 224 The surface area and length of the inner opening 224 223 is substantially smaller than the length of the closed edge curve 223, thereby forming at least one region 231 of the inside low-lying surface 103 of the closed envelope 224 where the closed curve 224 does not coincide with the edge curve 224.
In the arrangement according to Fig. 1b, according to a preferred embodiment of the present invention, the closed edge curve 223 of the opening coincides with the closed edge curve 227 defining the low ejection surface 103. A preferred embodiment of said opening 203 is arranged in a narrow and linear fashion. Preferably, the narrow linear opening may be provided as an opening of less than 100 µm in the low emptying surface 103.
Definition of plane wave
An electromagnetic wave propagated far enough away from the transmitter, or more precisely, the discrete frequency components contained therein, may be treated as a plane wave. In a propagating plane wave, the electric and magnetic field vectors are perpendicular to one another, and they oscillate in the direction of propagation, the so-called. In a plane perpendicular to the poynting vector. The relationship between electric and magnetic field intensities is described by wave impedance. Usually, the electromagnetic signal from the base station to the outer shell of the building can be thought of as a plane wave 301 (Figure 1a), although reflections from the surrounding area outside the wall may modify the characteristics of the signal.
The plane of polarization of the plane wave 301 is defined according to the electric field vector 308 it comprises. The plane wave 301 may comprise an electric field vector 308 'oscillating in the first polarization, and may further comprise an electric field vector 308' oscillating in the second polarization, wherein the electric field vectors oscillating in the first and second polarization
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308 'and 308' are crossed. Further, in the first and second polarization, the oscillating electric field vectors 308 'and 308' may be mutually orthogonal.
The plane wave 301 'can be defined as the plane wave 301 whose electromagnetic energy is determined by the interaction of the electric field vector 308' oscillating in the first polarization with the oscillation of an orthogonal magnetic field.
The plane wave 301 "can be defined as the plane wave 301 whose electromagnetic energy is determined by the interaction of the oscillating electric field vector 308" with the oscillation of an orthogonal magnetic field.
The plane wave 301 may comprise two electric field vectors 308 'and 308 "oscillating in a cross polarization, wherein the plane waves 301' and 301" illustrate the propagation of the polarized wavefronts in the first and second polarization, and these may proceed in parallel.
The plane wave wavefronts 301 'and 301' may also arrive in independent directions, whereby either plane wave wavefront 301 'or 301' may more generally be described by plane wave 301.
Electromagnetic wave polarization
The level of polarization of an electromagnetic wave is defined by the vibration level of the electric field of the wave. The polarization of the wave can be either linear, elliptical, cross or circular polarization. Linear polarization comprises a single direction of oscillation of a dominant electric field in which the amplitude of the cross-polarization component 30 is significantly smaller. In elliptic polarization, the electric field comprises the direction of oscillation of the electric field which is perpendicular to the Poynting vector, as well as the direction of oscillation of the electric field which is smaller than this. The intensities of the two polarization components are described by the so-called iso-axis and minor axis 35 components. In practice, few radio transmissions remain purely li
20185840 prh 08 -10-2018 non-linearly polarized, even if transmitted as multiple path reflections, refractions and diffractions modify the characteristics of the signal along its path.
In cross-polarization, the wave typically carries two orthogonally oscillating electric field components. This is a particularly important form of polarization in modern telecommunication applications, since two orthogonal polarizations are capable of transmitting almost non-correlated communication channels simultaneously.
A more special form than cross polarization is circular polarization. Circular polarization comprises two electric field vectors, typically of equal amplitude, and waves of the same information transmitted with a 90 degree phase difference. The electric field of a circularly polarized wave rotates as the wave propagates, and the direction of rotation of the 15 waves depends on the sign of the phase difference of the summing polarization components. The two circularly polarized transmissions may be crosswise with their opposite directions of rotation. Fully orthogonal circular polarizations are uncorrelated.
A circularly polarized transmitter may be formed, for example, by two orthogonal, linearly polarized antennas, or an array of antennas having separate polarization components divided by the same message signal, e.g., a power divider, and implementing a 90 ° phase difference between the subcomponents. An alternative way of implementing the phased subcomponents 25 of a circularly polarized transmission is, for example, to use a hybrid that performs both splitting and phasing with the same component. Also, a circularly polarized antenna can provide a circularly polarized transmission without splitting the signal before the antenna. Thus, the antenna element itself is capable of forming two orthogonal polarization components of the same signal, and has a phase difference between them.
Particularly in ΜΙΜΟ and diversity applications, the transmitting levels of linear cross-polarization at the base station antennas are the polarization levels of -45 ° and + 45 °, which can transmit transmissions orthogonal to each other. In addition, utilization of orthogonal circularly polarized transmissions35 in wireless signaling is particularly effective.
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For example, the so-called narrow antenna beams. Massive ΜΙΜΟ technology could also utilize orthogonal circularly polarized signal currents.
Electromagnetic diffraction from aperture (narrow vs. wide aper5)
For clarity, an aperture 201 that transmits a radio signal is defined. Aperture is generally understood as any aperture or aperture. In this connection, the radio-transmitting aperture 201 on the low-emptying surface 10 103 comprises an area delimited by a closed curve 230, wherein said radio-transmitting aperture 201 is within said closed curve 230 and having a closed area 230 surface area of boundary curve 227, and which, when passed, is subjected to an electromagnetic signal ko15 of substantially lower transmittance than areas outside the aperture in the same material or structure.
The radio signal-transmitting aperture 201 on the low-emptying surface 103 comprises an area which further comprises mechanical or artificial methods 20 for enhancing the transmission of the electromagnetic signal. An artificial method in this context is to utilize the energy contained in the electromagnetic signal by interfering with the electrical conductor surface formed on the low-emitting surface 103 to create concentrated radiation sources 303 which are activated as radiation sources by the energy supplied by the electromagnetic signal. These new radiation sources emit electromagnetic energy to the shadow side of the low-emitting surface 103 to enhance the passage of the electromagnetic signal through the Building Material. When encountered, the electromagnetic signal of the low-emitting surface 103 passes through the aperture 201 formed therein with a significantly lower transmission resistance than when passing the low-emitting surface 103 from the outside of the radio-transmitting aperture 201.
Fig. 1a illustrates a radio-transmissive aperture 201 according to a preferred embodiment of the present invention, formed by a gap radiator array 202 formed by slit radial openers 207 consisting of narrow linear openings 203
20185840 prh 08 -10-2018 to enhance the passage of the electromagnetic signal through the Building Supply. Said gap aperture radiators 207 of said aperture 201 are arranged to form concentrated radiation sources emitting at least a first polarization electric field vector 308 ', and a second polarization oriented electric field vector 308' emitting concentrated first and second polarization mutually.
Said radio-transmitting aperture 201 defines for building material 110 an area delimited by a closed curve 230, wherein said radio-transmitting aperture 201 is within said closed curve 230 and has a surface area limited by a closed edge 230 that is substantially smaller than the periphery area of the area.
Figure 1b illustrates in more detail the slit radiator array 202 shown in Figure 1a, wherein said closed edge curve 223 of said opening 203 is arranged to resonate and receive electromagnetic energy comprised by a first polarization electric field vector 308 'with a first electric frequency slot radiator 207 '' at first operating frequency. Said gap radiators 207 'and 207' 'form a dual-polarized gap radiator array operating at a first frequency.
Figure 1b further illustrates a second operating frequency gap radiator array comprising gap electromagnetic energy receiving gap radiators 207 "comprising a second polarization electric field vector 308".
Figures 2a-2d show an insulating glass element 100 comprising at least two glass sheets 102, an intermediate space 105 between them, and at least one of which glass sheets 102 is provided with said low release surface 103.
Fig. 2a illustrates diffraction of an electromagnetic wave from a wide aperture, and Fig. 2c shows a diffraction of an electromagnetic wave in a narrow aperture according to an advantageous embodiment of the present invention, wherein said aperture 201 is arranged in a low emitting surface
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103, and the glass panels 102 are arranged as insulating glass element 100. Figure 2a illustrates the arrival of a plane wave 301 on a glass plate 102 comprising a low-emptiness surface 103 in a situation where a wide aperture is provided. A wide aperture refers to an aperture that is 309 in width. The wide aperture can be realized in this context, for example, as a planar frequency-selective filter 109, or by leaving the glass plate 102 uncoated.
Figure 2b illustrates, by way of example, a known planar frequency 10 selective filter 109 having a physical width 305 of electromagnetic signal-transmitting aperture of several wavelengths. In the case of the example of Figure 2a, the wireless communication devices 40T, 401 ", and 401" "located in an unknown state in the room, receive signal coverage only in random situations where the incoming electromagnetic level 15 wave 301 does not experience significant shading. In the case of the example, the wireless communication device 40T 'receives an obliquely incoming electromagnetic plane wave 301, but the out-of-range wireless communication devices 401' and 401 'are unable to establish a reliable wireless connection to the base station due to the narrow transmission sector 307.
Figure 2c illustrates an arrangement according to a preferred embodiment of the present invention, in which the first and second polarization oscillating electromagnetic energy received from plane 301 are re-emitted and efficiently applied to a room space wide beam transmission sector 307 utilizing narrow aperture diffraction.
The glass plate 102 to cover matalaemissiviteettipintaan 103 is formed narrow in width, preferably less than length a radio signal from the half-wavelength transmissive aperture 201 '(Figure 2d) the plurality of focused radiation source 30 303' a working slot radiator 207. The radio signal to cross the aperture 201 'is comprised by a slot radiator 207 is polarized in the direction of the first polarization, and is arranged to a gap radiator group which is activated as a radiation source by the electromagnetic energy transmitted by the electromagnetic planar wave 301 it receives.
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The glass plate 102 is formed to include matalaemissiviteettipintaan 103, a second narrow width, preferably less than half a length the radio signal wavelength permeable aperture 201, "a plurality of focused radiation source 303 'a working slot radiator 207'. The slit radiators 207 'comprised in the aperture 201' transmitting the radio signal are polarized to a first polarization in a direction perpendicular to the second polarization, and are arranged as a slit radiation group which is activated as a source of radiation by the electromagnetic level 301 of its received electromagnetic plane.
Figure 2d illustrates how the radio-transmissive aperture 20T implemented with slot radiators 207 and the radio-transmissive aperture 201 'can be implemented in a structure similar to a preferred embodiment of the present invention, wherein the insulating glass element 100 in the polar aperture 201 ", where the first and second polarization are intersecting.
For the sake of clarity, a radio-transmitting aperture 201 is generally defined to depict either of the transmitting radio-transmitting apertures 201 'in the first polarization or the transmitting-to-aperture 201 in the second polarization. Similarly, the physical width 305 of the aperture is defined to represent the aperture width 305 'of either the first polarized polarization or the aperture width 305 of the second polarization.
The radio signal to cross the aperture 201 of the physical width 305 is preferably less than half a wavelength long. In order to obtain a narrow aperture diffraction pattern and to minimize radiation zeroes mi30 in the transmission sector 307, the incoming plane wave 301 must illuminate the entire radio signal aperture 201, advancing at most one wavelength 309 from the beginning of the first region To illustrate this, a non-limiting example of the 800 MHz frequency band with narrow apertures is e.g.
20185840 prh 08 -10- 2018 det 5mm, 10mm, 30mm, 50mm, 100mm, and 150mm. For clarity, it is noted that the physical width 305 of the radio-transmitting aperture 201 shown in Fig. 2d is defined parallel to the X-axis shown in the figure, and the length of the radio-transmitting aperture 201 is defined in the Y-axis 5, respectively. In order to achieve sufficient directivity, the height of the aperture 201 transmitting the radio signal must be at least one wavelength 309 of the operating frequency.
The radio-transmitting aperture 201 according to a preferred embodiment of the present invention comprises an edge curve 230 defining a bounded area from the low-emitting surface 103. Said region may be of any shape. A preferred form is a rectangle or an oval having a width 305 preferably less than one wavelength at the lowest operating frequency of the gap radiator array 202 comprising said aperture. The width 305 of said surface 15 may also be determined in a direction deviating from the horizontal plane, said aperture 201 deviating from a vertically oriented rectangle or oval. The length of said aperture can be determined somewhere other than the width 305 in a direction substantially longer than said width 305.
The narrow aperture diffraction pattern of the present invention is illustrated in Fig. 2c by a broad transmission sector 307, where the concentrated radiation source 303 depicts, depending on the context, "Comprising a concentrated radiation source 303" in which the first and second polarizations are crossed.
In the situation illustrated by the example, the wireless communication devices 401 ', 401 ", and 40T" in unknown directions in FIG. 2c are now more likely to have a sufficient connection to the base station because the energy from the base station signal is spread to wide transmit sector 307 based on narrow aperture diffraction.
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Now, the radio signal transmitting aperture according to the present invention, 201 to take advantage of the narrow aperture diffraction, and is preferably less than half the wave length to width 305. Refinements physical state that the aperture can also be a multi-band structure, or it can operate broadband speeds.
The preferred maximum aperture width is then determined by the lowest operating frequency wavelength 309.
The radio-transmitting aperture 201 of the present invention may comprise a plurality of concentrated radiation sources 303 adjacent to each other in the direction defined by the physical width 305 of the aperture 10. Thereby, the electromagnetic wave passing through the low ejection surface 103 forms an interference pattern that determines the behavior of the transmission sector 307. Two radiation from the source of the interference caused by the transmission sector 303 307 determined by the beam width can be considered as a broad, uniform, when focusing radiation sources, the distance 15 of the aperture width in the direction X is preferably maintained at less than half the wave length lengths. When the two radiation from the source is increased the distance between the half-wavelength spacing greater, the interference pattern begins to form a plurality of zero points and maximum points, and the number increases with the distance between the radiation sources increases.
Multiple zeroes in the transmission sector 307 would result in possible disconnections in the shadows. In addition, in a multiple zero and maximum transmission sector 307, the wireless communication device 401, when moving, could switch between base stations more often than in a state determined by a wide and flat transmission sector 307, which is accomplished by the building material of the present invention.
As one essential difference between the wide aperture and the present narrow aperture, the following may be mentioned. Preferably, the wavefront of electromagnetic planar wave 301 emitted from the horizon by the base station illuminates the area of aperture 201 transmitting the entire radio signal as it passes through the aperture of up to one wavelength 309, irrespective of whether the electromagnetic plane
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Plane wave excitation at low ejection surface
When the electromagnetic plane wave 301 encounters an electrically conductive low emissivity surface 103, some of the energy in the wave is reflected back in its upstream direction or 5 in other directions where the reflected wave front 306 continues to propagate, and some of the wave energy is converted to resistive losses.
Figures 1a and 1b, and 3a-3c, show the encounter of the wavefront of the electric 10 field vector 308 comprising the plane wave 301 with the low ejection surface 103. The oscillation period of the propagating wavefront electric field vector 308 is one wavelength 309. During one oscillation period, the phase angle of the electric field vector changes by 360 degrees. In the first polarization, the polarized planar wavefront 301 'comprises a wavelength 309', and in the second polarization the polarized planar wavefront 301 'comprises a wavelength 309'.
In a situation such as the one, preferably, the electromagnetic plane wave 301 arriving from the horizon arrives at a random azimuth angle 20 311. In the first polarization, the polarized plane wave front
301 'arrives at an azimuth angle 31T, and in another polarization, a polarized planar wave front 301' arrives at an azimuth angle 311 '.
The oscillating electric field of the incoming planar wave 301 causes at the same frequency a vibrational motion of electrons in the conductor surface. The motion of electrons is compressed on the outer surfaces of the conductor surface, forming a surface current pattern oscillating on the conductor surface. The surface current vector 214 in the conductive surface comprising the surface current is always perpendicular to the direction of the magnetic field parallel to the surface. On the surface of a complete electrical conductor, the electric field 30 in the direction of the surface disappears completely. The surface resistance of the non-ideal conductor surface converts some of the energy contained in the signal to heat due to resistive losses. This surface resistance depends on the low-ejection surface 103 in use.
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In the first polarization, the oscillating electric field vector 308 'induces a surface current vector 214' on the low-emitting surface 103. In another polarization, the oscillating electric field vector 308 "induces a low-current surface 103 on the surface current vector 214".
For the sake of clarity, define the azimuth angle parallel to the XZ plane and the elevation angle parallel to the YZ plane. incoming azimuth 311 of a plane wave 301 of electromagnetic energy induced pintavirtavektorit 214 form matalaemissiviteettipinnalla 103 flowing into the wide a wave 10 propagating electrons flow movement, which measure the flow pattern of oscillation is detected the incoming plane wave of wavelength 309 projection 310 matalaemissiviteettipinnassa 103. The incoming plane wave 301 electric field vector 308 determined by the plane of polarization of the amount of the primarily formed matalaemissiviteettipinnassa 103 pintavirtavektorien 214 oscillation directions15 nan. The polarization plane can be a vertical oscillation plane, a horizontal oscillation plane, or anything in between. The primary direction of travel of the wave pattern propagating as the oscillating surface current mat on the low ejection surface 103 is determined by the direction of incoming incoming planar wave 301. The he20 ray caused by the electromagnetic energy of the incoming plane wave 301 causes the vibration of the surface current vectors 214 in the low reduction surface 103 to be polarized by the incoming wave electric field vector 308. In addition to this polarization and direction of flow, the low-emitting surface 103 exhibits secondary surface current motion primarily caused by electron biasing induced by surface-induced surface current vectors 214. This is typically manifested as eddy currents, which mainly hate in areas that are not primarily illuminated by the electric field vector 308 of the incoming plane wave 301. Surface flow return current conventionally produces loop-like flow patterns.
The slit radiator array 202 formed by narrow radiation apertures 203 of the radio-transmitting aperture 201 of the present invention is based on appropriate interference with the flow paths of the surface current vectors 214.
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The narrow linear opening 203 of the present invention is arranged to effect an interference with the flow of the surface current vector 214 induced by the electric field vector 308 such that the first positive charge distribution 208 is formed at the narrow first opening 203 and the second and an electromotive force 204 acting in the non-conductive region of the narrow linear aperture 203 therebetween. The present electromotive force 204 acts as a central radiation source 303 for re-radiating electromagnetic energy into the shadow area of the insulating glass element 100.
A concentrated radiation source 303 comprising an electric field acting as a radiation source is arranged in the non-conductive region of the gap radiator 207, and this radiation source can be arranged as an effective radiator when said electric field 15 is arranged to resonate with the low-emitting surface 103. The first positive 208 and the first negative 209 charge distribution arranged on the low-emitting surface 103 serve as the source and hub of said surface current. Said charge distributions are formed by interfering with the low-emitting surface of electromagnetic 20 plane 301 on the flow of induced surface current vectors 214.
The radio-transmissive aperture 201 'of the present invention provided with a low-emitting surface 103 is arranged to receive and re-emit electromagnetic energy in a first polarization, wherein an electric field vector 308' comprising a first polarization provides an electro-electric The generated electromotive force 204 'is arranged to produce a resonant circuit together with an opening-circulating current loop 30 210' which acts as a polarized concentrated radiation source 303 'in the first polarization.
Said resonance in an electromagnetic system is generally referred to as an oscillation phenomenon in which the system interacts with its environment 35 and at some characteristic oscillation frequency is capable of receiving or
20185840 prh 08 -10-2018 to transmit electromagnetic energy. In electromagnetic resonance, the oscillating energy is alternately stored in the electrical and magnetic fields of the system. In the resonance of the gap emitter 207 formed on the low activity surface 103, the surface currents 5 formed at the edges of the gap emitter 207 are substantially in contact with the resonating magnetic field.
The radio-transmissive aperture 201 "provided in the low-emitting surface 103 of the present invention is arranged to receive and re-emit electromagnetic energy in a second polarization, wherein an electric field vector 308" comprising a second polarization provides a second-to- The resulting electromotive force 204 "is arranged to produce a resonant circuit along with an opening orbiting current loop 210", which provides 15 milliseconds as a polarized focused radiation source 303 ".
When the flow of the surface current vector 214 at the low emptying surface 103 is suitably disrupted by narrow linear openings 203, either by a break 20 bar or by redirecting the flow of current, a plurality of electromotive forces 204 are induced to benefit from interfering electromagnetic fracture propagation. This set of electromotive forces forms a gap radiator array 202 consisting of concentrated radiation sources 303.
Examining the effect of a single narrow linear opening 203 on the surface current vector 214, it can be seen that while the surface current induced electric field vector 308 continues to influence the conductor surface electron motion, the flow path 214 curves and forms a 203 is oriented orthogonally to the direction of the electric field vector 308 of the incoming planar wave 301. Such an opening provides two symmetrical current loops 210 rotating the opening 203, which rotate the narrow linear opening 203 on both sides thereof.
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The current loop 210 circulating the narrow linear opening 203 together with the electromotive force 204 forms a resonant circuit which enables the narrow linear opening to function as an efficient radiator. The dimensions of the narrow linear opening 203 are resonated at the operating frequency of the incoming electromagnetic energy carrier plane 301, whereby the narrow linear opening 203 effectively forms a radiating slit radiator 207 which re-radiates the electromagnetic energy received by the electromagnetic planar 301.
A narrow aperture of concentrated radiation sources emitting a coherent wavefront
202 comprising a radio signal transmitting aperture Rakosäteilijäryhmän 201 emits a wavefront based on the diffraction of the aperture of a narrow lähetyssekto15 its Rx 307. The radio signal to cross the physical width of the aperture 305 is preferably less than half a wavelength long. In this case, preferably arriving at the horizon transmitted by the base station electromagnetic plane wave 301 of the wave front illuminating the whole of a radio signal to cross the aperture 201 of the surface area of passes up to one, preferably a half-wave length distance of the aperture kohda20 when hot, regardless of whether or not an electromagnetic plane wave 301 matalaemissiviteettipinnan 103 normal direction or in substantially differing from the azimuthal angle.
The condition described above achieves a situation in which the electric field vector 308 of the incoming plane wave 301 illuminates the aperture through the radio signal almost simultaneously and in phase. This provides, within the aperture 201 transmitting the radio signal, a gap radiator array 202 which each individual gap radiator 207 comprises an oscillating electric motor force 204 in the same phase, in the shadow area on the opposite side of the insulating glass element 100.
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In the case of a wide aperture, single concentrated radiation sources are formed which do not oscillate in the same phase and whose emitted electromagnetic radiation does not form a coherent wavefront in the blind spot. The individual slit radiators of the wide aperture oscillate at different stages with respect to each other and therefore the reflection and radiation pattern produced by the wide aperture is strongly dependent on the incident angle of the electromagnetic plane wave that illuminates it. This is a typical technical feature, for example, with flat frequency-selective surfaces forming a wide aperture.
The present invention utilizes surface currents generated by planar waves on the low-emitting surface 103 to form new concentrated radiation sources 303 such that the electromagnetic wavefront emitted by the radiation sources is coherently summed on the opposite side of the low-emptying surface, The present invention thus permits the passage of an electromagnetic signal through a thermo glass element having a low emptying surface by creating a virtual aperture having an effective surface area greater than the physical openings formed on the low emptying surface. Furthermore, the insulating glass element 100 according to the present invention is capable of receiving electromagnetic energy from a maximum wide horizontal beam in space comprised by a plane wave.
Figures 3a and 3b show an example of a coherent wavefront generated by a plurality of focused radiation sources comprising a narrow aperture, wherein said aperture is arranged in conjunction with Building Material 110.
Fig. 3a is a top plan view of a coherent wave 30 30 arriving at the surface of an outer glass sheet 102 of insulating glass element 100 having a low-emptivity surface 103 formed on its exterior surface. and from which electromagnetic energy is provided as a coherent wavefront 302 formed on the side of the room.
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Figure 3b is a side view of the situation of Figure 3a. It can be seen that in the vertical direction the wavefront 302 spreads substantially at least at the height of the window, but in practice also in this direction is very wide and covers substantially the entire room in height, especially farther from the insulating glass element 100.
The redirected wave 304 emitted by the central radiation source 303 forms a mesh over the shadow area created by the insulating glass element 100.
The energy reception and re-emitting of the incoming electromagnetic wave through a plurality of concentrated radiation sources 303 is accomplished by carefully positioned narrow linear openings in the low emitting surface. As described above, the incoming electromagnetic wave generates surface currents in the electrically conductive coating. The direction of the surface currents in the conductor is determined by a 15 wavelength perpendicular to the magnetic field vector. When the direction of the formed surface currents is disturbed by the narrow linear openings 203 in the low-emptying surface, the surface current rotates the formed opening along its edges and creates a resonant circuit along with an electromotive force 204 20 acting over the narrow linear opening 203.
The building material 110 of the present invention may comprise a single radio-transmitting aperture 201 arranged to operate in one or more polarizations in one or more frequency bands. The building material 110 may also comprise a plurality of radio-transmitting apertures, the polarizations or operating frequencies of which may differ from each other. Furthermore, the present building materials can be used to implement wall or facade structures comprising a plurality of said radio-transmitting apertures 201, wherein the apertures 30 of said apertures are preferably arranged to be less than ten meters. Some advantageous distances between said apertures can also be, for example, 2 to 5 meters, or 1 to 2 meters, whereby isolation can be provided between the individual apertures to ensure the desired function.
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Coherent reception and transmission from multiple slot radiators
It is known that the efficiency of passive repeaters is poor. Factors contributing to this include heat loss in cabling between antennas and rapid attenuation of the electromagnetic energy emitted from the antenna element as a function of distance. This repeater efficiency can be improved in individual directions by using directional rake antennas, whereby antenna gain achieves improved efficiency in a narrow sector. The problem with such a repeater, however, is that its rake antennas 10, such as the Yagi antenna, must be pointing to a single base station. Rare antennas with narrow antenna beams do not receive signals efficiently from the side.
According to a preferred embodiment of the present invention, the horizontally wide reception and radiation beam provided by the diffraction pattern formed by the narrow radio-transmitting aperture 201 arranged on the ma15 surface 103 provides advantages over the design narrow-band antennas.
It is an object of the present invention to enhance the efficiency of a building material 110 acting as a passive signal transmission system by appropriate control of the energy of electromagnetic waves in a building material shaded area where an opening 203 is provided through a low emptying surface 103 to power the electromagnetic signal. Said electromagnetic signal comprises an incoming plane wave 301, and said building material passed electromagnetic signal comprises a redirected wave 304.
In addition to the horizontally wide receiving and radiation beam formed by the narrow aperture described above, another advantageous feature of the present invention is to increase the efficiency in a horizontally wide beam such that a plurality of concentrated in the shaded area formed by Building Material 110. Mai
20185840 prh 08 -10-2018, said wavefront of redirected wave 304 formed by summed electromagnetic waves is known as coherent wavefront 302.
The concentrated radiation sources 303 constituting the redirected waves 304 comprised by said coherent wavefront 302 may be arranged preferably at less than a wavelength distance apart, preferably in a vertical queue in which the queue can be either straight or meandering. As the distance between adjacent concentrated radiation sources 303 increases beyond the wavelength of the operating frequency 10, the number of side beams occurring in the formed radiation beam increases, thereby losing some of the electromagnetic energy to be transmitted in the undesired directions. Advantageously, the vertical array formed by said concentrated radiation sources can be arranged over the operating frequency to a wavelength, whereby an increase in the generated radiation and reception beam gain in the directions of use is achieved.
Fig. 4 illustrates a preferred embodiment of the Building Material 110 of the present invention, wherein said building material comprises at least one electrically conductive low level surface 103 having an opening 203 for enhancing the passage of the electromagnetic signal through the Building Material and having a lower electrical conductivity 10; the edge 203 of the opening 203 provided on the low ejection surface 103 forms at least one closed edge 25 curve 223, and said opening 203 defines a closed envelope 224 such that said opening 203 is inside the closed envelope 224 and has a surface area 22 the area and length of the inner opening 203 being substantially smaller than the length of the closed edge curve 223, thereby forming at least one closed curve 224 and a closed envelope 224 that does not coincide with the edge curve 223.
In the example of Fig. 4, a low-emissivity surface 103 is provided with at least 35 gap-radiating array 202 radiosig comprising two of said gap radiators 207
20185840 prh 08 -10-2018 for forming a transmissive aperture 201, wherein said gap emitters 207 are arranged to form concentrated radiation sources 303 emitting at least said first polarization direction electric field vector, and wherein said radio signal transmitting aperture 201 defines a building, wherein said radio-transmitting aperture 201 is within said closed curve 230 and having a surface area defined by a closed curve 230 that is substantially smaller than an area defined by a closed edge curve 227 defining a low-emptying surface 103.
In the example of FIG. and an internal electric field vector oscillating in the second polarization between the two edges of the opening 203, which, together with said surface current formed on the low-emitting surface 103, forms a resonant 20-sided crossed with each other.
A closed curve delimiting said aperture 201 transmitting a radio signal
The width 305 'of the region comprised by 230 in the first polarization may be preferably arranged below the operating frequency to a wavelength. Correspondingly, the width 305 "of the region of the closed curve 230 defined by said radio-transmitting aperture 201 may advantageously be arranged below the operating frequency to a wavelength.
Figure 4 illustrates, in accordance with an advantageous embodiment of the present invention, a gap radiator array 202 provided by a building accessory 110 with a low-emitting surface 103 having a plurality of narrow widths defined in the X-axis 34
20185840 08 -10- 2018 phr, preferably less than Delta-scale radio signal from the half-wavelength transmissive apertures 201 ', a plurality of focused radiation source 303' a working slot radiator 207. The slot radiators comprise 45 degree and -45 degree polarizations and are linearly polarized. Slit radiators 207 are thus 90 degrees to each other in mass. When the wave front arrives at the direction of the arrow 301 'indicated by the direction in which the electric field oscillates in the direction of arrows 308' with respect to the direction of propagation of the wavefront that is perpendicular to the direction of the electric field causes the opening of the opening direction of travel of the wavefront along the edges of the electric field. The other end of the opening is short-circuited, thereby providing a current loop 210 'surrounding the opening. Arrows 214 'illustrate the surface current vector generated by this electric field on the low-emitting surface 103 further away from the slot radiators. Similarly, arrow 301 "indicated by the incoming wave front in the direction of the electric field oscillates in the direction of arrows 308 'direction, the electric field causes the wave front in the running direction of the opening 15 around the edge of the opening of the electric field. This opening is an opening perpendicular to the previous opening with one end short-circuited. Thereby a current loop 210 "is formed in the vicinity of this second opening. The arrows 214 "depict the surface current vector generated by this second electric field on the low-ejection surface 103 farther from the slot 20 radiators.
In both of the above situations, a group of concentrated radiation sources 303 formed by individual slit radiators 207 forms an incoming plane wave 30T, 301 ", a coherent wavefront of electromagnetic energy in the overhead space of the building material 110 building.
The structure of the 4 matalaemissiviteettipintaan 103 is formed with a plurality of narrow, having a width preferably less than a half-wave length scale radiosig30 margin permeable apertures. These apertures 201 comprise apertures 203 in which apertures 203 rotate in the low-emptying surface 103 such that the open ends of each aperture are close to each other and have a narrow conductive region between them. The apertures of adjacent slit radiators are at an angle of 45 degrees to each other, whereby these slit radiators have +45 degree and -45 degree polarizations and are linearly polarized. Inner and outer half 103 matalaemissiviteettipinnan a short circuit effect. Narrow range of force of the electric field
20185840 prh 08 -10-2018 to those corners of the zero. This expands the bandwidth. The openings serve as concentrated radiation sources 303 '. Which polarization the aperture is capable of receiving and further emitting depends on the direction of the electric field of the incoming wavefront with respect to the location of the o05 passage in the aperture, i.e. how the electric field is formed around the aperture.
When the wavefront comprises an aperture polarized oriented electric field vector, the aperture 203 is activated as a concentrated radiation source 303 polarized according to the electric field vector 308 illuminating it. Instead, the electric field polarized in a direction perpendicular to this direction does not provide a corresponding electric field around the opening.
Arranging a narrow, linear opening
The narrow linear opening at low emptying surface 203 may be defined as a bogie opening at an electrically conductive surface of a low emptying surface where the opening at the electrically conductive surface causes substantial electrical conductivity loss in the opening region and wherein the opening comprises an edge two sections of the boundary curve selected. By way of example, but not exclusively, it may be mentioned that the narrow linear opening can be, for example, 10 to 100 µm wide and 20 to 50 mm long, for example. The width of the narrow linear opening may also be 0.5 to 2 mm, for example. In addition, some mechanical means may have a narrow linear opening width of 5 to 10 mm.
In geometry, a point is a dimension that has a place but no dimension. When a non-conductive physical point, such as a narrow cutter blade, or a single pulse laser pulse is formed on the shallow cavity surface 103, a non-conductive area with a practically interpretable surface and a periphery is formed on the surface. For example, a single point produced by a pulsed laser may be of the order of micrometers or tens of micrometers in diameter, or less, depending on the technique used, such as a femtolaser or a nano laser.
A point moving in space forms a line. The line can be either straight, or it can be meandering or curved, or it can consist of several straight sections
20185840 prh 08 -10- 2018 broken line. The line may have a start and end point, or it may form a closed circle of arbitrary shape. Special cases of such an arbitrary closed circle include, for example, a circle, an oval, a square, a rectangle, a triangle, and polygons. The line can also cut itself.
A line or combination of lines may be used to control the device to provide the opening 203 of the low-ejection surface 103. For example, the focal path of a milling or pulsed laser focal point may be guided by a linear path, as may a chemical or other method or device provided for a contactless dry or removal method. Similar control can prevent the conductive surface from forming in the desired areas prior to providing the low-level surface 103 with the building material 110.
A physical point moving in space, such as a laser focal point, also includes a circumference and a surface. By way of example, but not exclusively, a circumference of 100 µm may be mentioned. As the exemplary physical point moves along the low ejection surface 103, it defines a narrow, linear opening 203. The opening has a closed edge curve 223, as well as the area delimited by this. Slit radiator 207 comprising opening 203 may be located inside closed edge curve 223. Slit radiator 207 comprising aperture 203 may also be located outside closed edge curve 223 if said closed edge curve forms a boundary curve 227 defining a low edge surface 103.
The two opposite edges of a straight line, such as a laser-etched opening 203 on a low-emptying surface 103, are generally parallel and define a rectangular opening if the rounding of the edges is not specifically considered. However, the two opposed edges 30 of the opening 203 need not be parallel or identical, but may be arbitrary. For example, the straight edge portion on the opposite side of the opening may be curved, meandering, or, for example, serrated. Thus, the width of the electrically non-conducting region of opening 203 may vary in different sections thereof. The opening 203 may have a plurality of edge 35 curves, such as, for example, Y or T-shaped openings that intersect the low edge surface from one edge to another.
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In this context, a non-conductive area refers to a substantially non-conductive area. In fact, there is no boundary between perfect conductor and perfect insulation, since almost all materials have some electrical conductivity, even if very low.
In practice, for example, copper, silver, aluminum, and selective surfaces with a surface resistance of less than 400 Ω / square can be interpreted as conductors, whereas, for example, wood, PVC, and glass are known as typical non-conductive insulators. However, a selective surface with a surface resistance of more than 100 Ω / square is in fact already a poorly conductive conductor, the antennas formed having 10 already very low radiation efficiency, whereas, for example, 1-10 neli / square surface resistive selective surfaces can be practically Good antennas are already obtained from 100 mΩ / square surface-selective membranes. When the surface resistance is close to the wave impedance of the free space, the conductor surface behaves like a planar resistor, whereby it effectively converts the energy of the electromagnetic signal into heat.
The opening 203 in the low-ejection surface 103 may be defined as an opening in the electrically conductive surface of the low-ejection surface, wherein said opening 20 causes substantial electrical conductivity loss in the opening region, and wherein the opening 203 comprises a closed directionally selected two sections of the edge curve. It is mentioned by way of example, but not by way of example, that a narrow linear opening can be, for example, 10 to 100 µm wide and 20 to 50 mm long, for example. The width of the narrow linear opening may also be 0.5 to 2 mm, for example. In addition, some mechanical means may have a narrow linear opening width of 5 to 10 mm.
An opening 203 according to a preferred embodiment of the present invention is arranged as a radio-transmissive aperture such that the opening is provided in a meandering or curved shape that interferes with the flow of the surface current vectors 214 formed at the low and that said opening 203 defines a closed envelope 224 such that said opening 203
20185840 prh 08 -10-2018 is within the closed envelope 224 and has a surface area defined by the closed envelope 224 substantially larger than the area and length of the inner opening 203 of the closed envelope 224 and substantially smaller than the length of the closed edge curve 223, a low emptying surface within the area delimited by closed envelope 224
103 region 231, at which closed envelope 224 does not coincide with edge curve 223.
The narrow linear opening can be accomplished by any method suitable for the purpose 10, but conventional methods include mechanical machining, such as grinding. Other methods include laser treatment or a chemical method such as etching which substantially weakens the electrical conductivity of the electrically conductive coating. By way of example, a method is mentioned in which the electrical conductivity of the coating is reduced by printing the desired pattern on a low surface area and then burning the pattern at high temperature.
The building material 110 of the present invention comprises at least a low edge surface 103 defined by a closed edge curve 227 and an opening 203 provided on said low edge surface 103, wherein said opening is delimited by at least one closed edge curve 223. it may form an independent boundary curve from this boundary curve (227). Preferably, said opening 203 has a surface area of at most one percent to 25 percent relative to said low surface area 103.
Figures 5a-5c show examples of building materials 110 in accordance with some preferred embodiments of the present invention.
Fig. 5a shows a building accessory 110 according to a preferred embodiment of the present invention, wherein the building accessory is an aluminum surface heat insulating panel comprising at least one electrically conductive low-emitting surface 103 having an opening 203 to enhance electromagnetic signal flow through the building material low level surface 103.
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In the exemplary embodiment of Figure 5a, the edge of said opening 203 disposed on the low ejection surface 103 forms at least one closed edge curve 223, and said opening 203 defines a closed envelope 224 such that said opening 203 is inside a closed envelope 224 and 5 has a closed envelope substantially larger than the area 226 of the inner opening 203 of the closed curve 224 and substantially less than the length of the closed edge curve 223, thereby forming at least one area 231 with.
An exemplary building material 110 of Fig. 5a comprises a low-ejection surface 103, wherein the closed edge curve 223 of the opening 203 is arranged to coincide with the closed edge 15 delimiting the low-ejection surface 103. Said low ejection surface 103 is disposed on a surface of dielectric material 229, wherein said dielectric material is delimited by a closed edge curve 228. Said dielectric material is a heat insulating material preferably having a density less than 200 kg / m 3. The materials of said thermal insulation material may be, for example, EPS, XPS, PIR20 or PUR foams, or similar dielectric materials made of plastic. Said low-emissivity surface 103 may be provided, for example, with an aluminum coating.
The low-emitting surface 103 of Fig. 5a comprises an opening 203 arranged to form at least one positive 208 and negative 209 charge distribution acting as poles of a low-current surface 103 as an electric field vector which, together with said low-emitting surface
103, with a surface current formed, forms a resonant circuit for generating a gap radiator 207 operating in the first polarization as a concentrated radiation source 303 which enhances the passage of the electromagnetic signal through the building material.
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The closed edge curve 223 of the exemplary opening 203 of Figure 5a comprises a first edge curve portion 221 and a second edge curve portion 222, wherein the first edge curve portion 221 is arranged to be meandering. The width of said opening 203 is not uniform but varies as a function of position. Arranging said portion of the curve of the edge curve provides beneficial effects on the operation of the slot radiator 207. The meandering curve portion 221 acts to extend the flow path of the resonating surface current 210 formed on the low ejection surface 103, whereby the resonant dimension 215 of the opening 203 lengthens and the resonance frequency of the opening 203 shifts to lower frequencies. This 10 has the effect of reducing the size of the opening 203, since the frequency offset is usually compensated by reducing the size of the gap radiator 207. Correspondingly, this has the effect of reducing heat loss on the low-emitting surface 103. The maximum of the resonating current loop 210 is typically located within the short-circuit end 205 of the opening 203. In many cases, the open end region 206 of the opening comprises the maximum value of the electric field defining the electric motor force formed inside the opening. Said open end 206 can be formed if the closed edge curve 223 of the opening is arranged to coincide with the closed edge curve 227 delimiting the low activity surface 103.
Arranging at least one edge of the opening to curve can improve the radiation properties of the slot radiator 207, since increasing the closed envelope 224 delimiting the opening 203 affects impedance matching and bandwidth, as increasing the opening 203. Furthermore, arranging said edge curve to meander may cause new resonances in the opening to new frequency bands 25, or new polarizations, whereby a single opening 203 may be provided with a plurality of concentrated radiation sources 303 for different frequency bands and different polarization components.
The low emitting surface 103 of Fig. 5a is provided with a plurality of slit radiators 207 comprising two said slit radiators 207, wherein the concentrated radiation sources 303 comprised by said slit radiators 207 are arranged in a vertical row. The vertical distance of said two adjacent focused radiation sources 303 is preferably arranged to be at most one wavelength at the lowest resonance frequency of said slit radiators 207, and said vertical array may be preferably straight or meandering.
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Figure 5b illustrates a building accessory 110 according to a preferred embodiment of the present invention, comprising at least one electrically conductive low-emitting surface 103 having an opening 203 for enhancing the passage of an electromagnetic signal through the building material and having an opening having a substantially lower conductivity than in the embodiment, the edge of said opening 203 arranged on the low-facing surface 103 forms at least one closed edge curve 223, and said opening 203 defines a closed envelope 224 such that said opening 203 is within the closed envelope 10 224 and bounded by the area 224 of the closed envelope.
225 is substantially larger than the area 226 of the inner opening 203 of the closed curve 224 and substantially less than the length of the closed edge curve 223 to form at least one area 231 of the low-emptying surface 103 within the area delimited by the closed curve 224. with edge curve 223.
An exemplary building material 110 of Fig. 5b comprises a low edge surface 103, wherein the closed edge curve 223 of the opening 203 is arranged to form a closed edge curve separated from the closed edge curve 227 defining the low side surface 103.
The low-ejection surface 103 of Fig. 5b comprises an opening 203 arranged to form at least one positive 208 and negative 209 charge distribution acting as poles on the low-ejection surface 103 as a result of a first polarizing an electric field vector which, together with said surface current formed on the low-emitting surface 30103, forms a resonant circuit for generating a gap radiator 207 operating in the first polarization as a concentrated radiation source 303 which enhances the passage of the electromagnetic signal through the building material.
The closed edge curve 223 of the exemplary opening 203 of Figure 5b comprises a first edge curve section 221 and a second edge curve section 222 where
20185840 prh 08 -10-2018, both the first edge curve part 221 and the second edge curve part 222 are arranged to be meandering. The width of said opening 203 is not uniform but varies as a function of position. Arranging said edge curve portions to meander will provide beneficial effects on the operation of the slot radiator 207. The meandering portion of the curve effects the flow path of the resonating surface current 210 formed on the low ejection surface 103, whereby the resonant dimension 215 of the opening 203 becomes longer and the resonance frequency of the opening 203 shifts to lower frequencies. This has the effect of reducing the size of the opening 203, since the frequency offset is usually compensated by reducing the size of the slot radiator 207. Correspondingly, this has the effect of reducing heat loss on the low-emitting surface 103.
Fig. 5c illustrates a building accessory 110 according to a preferred embodiment of the present invention, wherein the building accessory comprises at least one electrically conductive low-emptying surface 103 provided with an opening 203 to enhance the passage of the electromagnetic signal through the building material and having an electrical conductivity substantially lower than in an exemplary embodiment, the edge 20 of said opening 203 provided on the low edge surface 103 forms at least one closed edge curve 223, and said opening 203 defines a closed envelope 224 such that said opening 203 is within the closed envelope 224 and has a closed envelope 224 than the area 226 and the length of the inner opening 203 of the closed envelope 224 is substantially smaller than the length of the closed edge curve 223, thereby forming at least one area 231 of the low ejection surface 103 of the area enclosed by the closed curve 224, at which the closed curve 224 does not coincide with the edge curve 223.
The exemplary building material 110 of Fig. 5c comprises a low ejection surface 103, wherein the closed edge curve 223 of the opening 203 is arranged to coincide with the closed edge curve 227 defining the low ejection surface 103. Said low ejection surface 103 is disposed on the surface of the dielectric material 229, wherein said dielectric material is bounded by a closed edge curve 228.
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The closed edge curve 223 of the exemplary opening 203 of Figure 5c comprises a first edge curve section 221 arranged to be meandering. The width of said opening 203 is not uniform but varies as a function of position. Arranging the said curve portion of the curve provides beneficial effects on the operation of the slot 207. The meandering curve portion 221 acts to extend the flow path of the resonating surface current 210 formed on the low-emitting surface 103, thereby extending the resonant measure 215 at different frequencies of the opening 203 and shifting the resonant frequency of the opening 203 to lower frequencies. This has the effect of reducing the size of the opening 203, since the frequency offset is usually compensated by reducing the size of the gap radiator 207. Correspondingly, this has the effect of reducing heat loss on the low-emitting surface 103.
The maximum of the resonating current loop 210 is typically located in the region of the transported end 205 of the opening 203 to 15 at a single resonant frequency. In many cases, the area of the open end 206 of the opening comprises the maximum value of the electric field defining the electric motor force 204 formed inside the opening. Said open end 206 may be formed if the closed edge curve 223 of the opening is arranged to coincide with the closed edge curve 227 delimiting the low ejection surface 103 20.
Arranging at least one edge of the aperture to curve may improve the radiation properties of the slot radiator 207, since increasing the closed envelope 224 delimiting aperture 203 affects impedance matching and bandwidth 25 as increasing aperture 203. Furthermore, arranging said edge curve to meander may cause new resonances in the opening to new frequency ranges, or new polarizations, whereby a single opening 203 may be provided with a plurality of concentrated radiation sources 303 for different frequency ranges and different polarization components.
5c, a plurality of said radiation sources 303 having different operating frequencies and polarization levels are provided in a low emitter surface 103 according to a preferred embodiment of the present invention.
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Operation of a single narrow linear opening as a concentrated radiation source
An arrangement such as a preferred embodiment of the Building Material 110 of the present invention comprises a gap emitter array 202 provided on a low emptying surface 103 formed by narrow linear apertures on a low emptying surface 203 and wherein a a sonar circuit serving as a concentrated radiation source 303.
Figures 6a-6c show some openings 203 according to some preferred embodiments of the present invention in the low-emptiness surface 103. Figure 6a illustrates an example of a gap-emitter 207 provided in the present invention 15, and another exemplary embodiment of the present invention. 6c illustrates how the solution illustrated in Fig. 6b can be arranged on a low-emptying surface 103, for example, by a single laser-fired meandering 20 or branching line.
6a-6c, it is typical that the opening 203 provided on the low-emitting surface 103 enhances the passage of the electromagnetic signal through the building material and that the electrical conductivity of said opening is substantially lower than the electrical conductivity of said low-emitting surface 103. It is also typical of said opening 203 that the edge of the opening 203 forms at least one closed edge curve 223, and said opening 203 defines a closed envelope 224 such that said opening 203 is within the closed envelope 224 and has a bounded area 225 of the closed envelope 224. substantially larger than the closed envelope
The area 226 and the length of the inner opening 203 223 are substantially smaller than the length of the closed edge curve 223, thereby forming at least one area 231 of the inner low surface area 103 of the closed envelope 224 where the closed curve 224 does not coincide with the edge.
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6a-6c, it is also typical that the aperture 203 provided on the low emptying surface 103 is arranged to form at least one positive distribution 208 and a negative 209 charge distribution on the polarity, an electric field vector oscillating in the first polarization between the two edges which, together with said surface current formed on the low-emitting surface 103, forms a gap radiation 303 acting as a concentrated radiation source 303 which enhances the passage of the electromagnetic signal 10 through the building material.
Fig. 6a illustrates a preferred embodiment of a slot radiator 207 of the present invention, wherein a narrow linear opening 203 is arranged to provide a first positive charge distribution 208, and a first negative charge distribution 209 at the edges of a narrow linear opening and an opening 203 in an area of non-conductive bounded by an edge curve.
6a, the, present formed by a slot radiator according to the preferred embodiment of the invention the narrow line-shaped similar to the opening 203 of the resonance circuit 207 comprised by the resonant dimension 215 is preferably arranged at the incoming side of a plane wave length 301 värähtely25 frequency. Preferably, said resonant circuit of said gap emitter 207 may be resonant at some frequency between 600 MHz and 6000 MHz. Preferably, said resonant circuit of said slit radiator 207 may also be resonant at some frequency between 300 MHz and 30 GHz.
Fig. 6b illustrates a preferred embodiment of the slot radiator 207 of the present invention, wherein a narrow linear aperture 203 is arranged to provide a first positive charge distribution 208, and a first negative charge distribution 209 at the edges of a narrow linear aperture, a line opening 203 in a region delimited by an electrically non-conducting region.
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The electromotive force 204 of the gap radiator and the associated current loop 210 form a resonant system oscillating at the resonant frequency. Preferably, said resonant frequency can be provided for one or more frequencies in the range of 300 MHz to 30 GHz.
The arrangement shown in Fig. 6b according to a preferred embodiment of the present invention also comprises an area within the low curvature surface 103 in the area delimited by an edge curve of a narrow line region 203 arranged to form a second positive charge distribution 211 and a second negative charge distribution 212. two electromotive forces 204 which individually function as concentrated radiation sources 303 and whose induced electromagnetic radiation forms a coherent wavefront 302 propagating in the blind area.
The 6b presented by the resonant dimension 207 comprised by the slot radiator formed by a narrow line-shaped according to a preferred embodiment of the throw of the present invention 203 215 are preferably arranged at the incoming side length of a plane wave 301 of the frequency of vibration.
An embodiment of a preferred embodiment of the present invention offsets the efficiency loss typically caused by low conductivity low surface area losses by arranging differential current generating portions of low surface area openings 203 so that the efficiency is reduced by the currents. Said reversible currents are formed in close proximity to the same low conductivity surface conductive region so that they are not significantly separated by an opening arranged between the currents.
The examples of Figures 6a and 6b further mention a region delimited by an edge curve of a narrow linear region 203 arranged to form a second positive charge distribution 211 and a second negative charge distribution 35 212, wherein the arrangement illustrated comprises two electric motor forces 204 which individually function as concentrated radiation sources 303 induced
20185840 prh 08 -10-2018, the electromagnetic radiation forms a coherent wavefront 302 propagating in the shadow area. The examples further illustrate a return current 213 formed between the second positive charge distribution 211 and the second negative voltage charge 212. The flow direction of said return stream 213 in the examples of Figures 6a 5 and 6b is opposite to the direction of flow of current loop 210. Said return current 213 forms a differential, i.e., differential, surface current in a gap radiator such as that shown in Figures 6a and 6b, wherein current loop 210 and return current 213 flow in opposite directions close to one another. A transmission line carrying converging currents, such as the narrow opening section 10, does not constitute an effective electromagnetic energy radiator, and as shown in FIGS. 6a and 6b, and between 211 and 209. In the arrangements of Figures 15 6a and 6b, the currents 210 and 20 flow in opposite directions
213 form a differential pair, in which the differential currents are concentrated in a portion of the gap radiator 207, where the current is concentrated at the edges of the opening 203, and where the surface current travels in an electrically conductive region of low shallow surface 103.
6a and 6b, the gap radiator 207 described herein comprises two focused radiation sources 303, wherein said radiation sources 303 comprise portions of opening 203 of a low-emptying surface 103, where the elements are determined by the current 210 and the return current 213, and wherein the differential current elements appearing on the low ejection surface 103 comprise portions of the opening 203 arranged in overlap. Fig. 6a illustrates a differential current element 232, as well as its reverse 30 differential current element 233, wherein said differential current elements occur in a portion of the gap radiator 207 and wherein said currents occur at electrically conductive edges of opening 203 with said edges each other.
Said differential currents comprise a differential current element 232 as well as a reverse current element flowing near said current element 232
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233. In the structure shown in Fig. 6a, the distance of said differential currents is determined by the width of the opening 203 at the portion in which said currents are formed by an external excitation. Typically, the opening 203 may have a width of, for example, 105 to 100 µm on a single laser line, or, for example, open on a laser, may have a width of, for example, 0.1 to 2 mm. In addition, some mechanical means may have a narrow linear opening width of 5 to 10 mm.
The closed edge curve 223 of the exemplary opening 203 of Figure 6b comprises a first edge curve portion 221 and a second edge curve portion 222, wherein both the first edge curve portion 221 and the second edge curve portion 222 are arranged to be meandering. The width of said opening 203 is not uniform but varies as a function of position. Arranging said edges of the curve provides a beneficial effect on the electrical operation of the slot radiator 207. The meandering portion of the curve causes the resonant surface current 210 formed on the low ejection surface 103 to extend the flow path, whereby the resonant dimension 215 of the opening 203 becomes longer and the resonant frequency of the opening 203 shifts to lower frequencies. This has the effect of reducing the size of the opening 203 because the frequency offset is usually compensated by reducing the size of the gap beam 207. Accordingly, this has a low ejection surface
103 loss of heat.
Figure 6b illustrates how, in an embodiment such as a preferred embodiment of the present invention, a curved portion of the opening curve 25 can be applied to extend the flow path of the current loop 210. In addition, a special phenomenon improving the electrical operation of the gap radiator is achieved by the fact that the current stream loop 210, as well as the return stream 213 flowing in the region of low emptying surface delimited by another edge of opening 203, can be forced to flow farther apart. This phenomenon has a particularly beneficial effect on the efficiency, bandwidth, and resonance control of the impedance in the gap radiator. The adjustment of said impedance is further influenced by an electromotive force inducible inside the opening 203, the position and intensity of which can be controlled by arranging some edge curve of the opening. The above-mentioned 35 phenomena in which the efficiency and bandwidth of the gap radiator is improved can be explained by the fact that typically in the opposite direction, i.e.
20185840 prh 08 -10- 2018 hate, ns. differential currents, are not efficient radiators if opposing currents travel close to each other. By interfering with the differential surface current as described in the example, the function of the structure as a radiator can be enhanced.
6b and 6c, wherein the edge of the opening 203 comprises a section arranged to be curved such that the low-emptying surface 103 is delimited by the low-emptying line 10 of the area bounded by the closed curve 224 with an electrically conductive region 231 the surrounding closed curve 224 is not coincident with the closed edge curve 223 of the opening 203. Said region 231 may advantageously be arranged such that the edge curve portion 221 defining the electrically conductive region 231 defines two or more opening portions arranged at least partially overlapping.
Said sections are arranged at a distance 234 from each other where the distance
234 limits the distance between the differential current elements formed in the electrically conductive region 231, wherein said differential current elements travel at opposite edges of the continuous conductor region. In an arrangement according to a preferred embodiment of the present invention, said distance 234 is arranged to be less than one tenth of the wavelength of the operating frequency. By way of example, for example, with active slot radiators in the 800 and 900 MHz bands, differential current elements arranged less than 50 mm apart begin to interact, and within each other the hate effect is already significant. When the differential current elements 234 are less than 5 mm apart, the opposite current elements 232 and 233 within the region 231 delimited by the overlapping portions of the opening 203 overlap each other, and the surface current in the direction of the current current 210 is amplified in said conductive regions.
In a preferred embodiment of the invention, said at least one opening 203 is arranged to form an electric field such that said at least partially overlapping edges are overlapping in the direction of the electric field acting over the edges.
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Figure 6b illustrates the formation of differential current elements 232 and 233 in portions formed by portion 221 of the edge curve of opening 203, wherein the edge portions of opening 203 are arranged partially overlapping. The electromagnetic energy carried by the incoming planar wave 301 acts as an excitation for opposite charge distributions formed at the edges 203 of openings 203 arranged on the low-emissivity surface 103. Said charge distributions serve as sources for surface current 210, said surface current 210 dividing into a common and differential current mode by a closed envelope 224 defining a radio-transmissive aperture 201 comprising a low-emptivity surface 10 103. In Fig. 6b, for illustrative purposes, differential current elements 232 'and 233' are distinguished from other marked current elements 232 and 233. Said current elements 232 'and 233' form a stronger amplitude than the other said current elements 232 and 233, the embryos are arranged mutually mutually disposed in a construction according to a preferred embodiment of the present invention. The arrangement shown now causes a portion of the meandering edge curve 221 to behave like a wide opening in a low ejection surface. The present arrangement improves the efficiency and bandwidth of the narrow linear aperture 203, which acts as a slot emitter, especially when the aperture is less than 500 µm, and when the aperture is implemented on a low-emptying surface which acts as an unidirectional electricity20.
Fig. 6c further illustrates the implementation of an opening 203 similar to the example shown in Fig. 6b by means of a device for producing a narrow linear opening, such as a laser. The opening 203 may be provided on the lower surface of the civic surface 103 preferably using a single curved or branched line. Preferably, said line may be less than 200 µm wide.
Vertical polarized gap radiators in a conductive grid structure
The narrow linear opening 203 according to a preferred embodiment of the present invention may be used to enhance the passage of the electromagnetic energy of the level wave 301 through the electrically conductive lattice structure 220. The electrically conductive lattice structure220 may comprise metal blinds. The electrically conductive grid structure 35 may also comprise a second low ejection surface 103
20185840 prh 08 -10- 2018 frequency selective surface. Figures 7a-7c show an example of such a structure.
Typically, the horizontal blinds comprise a plurality of thin metal strips 216, the position 217 of which can be rotated to adjust the amount of light transmitted through the window. Metal blinds are known to interfere with the passage of electromagnetic energy through a window. For example, U.S. Pat. No. 5,346,485A to Central Glass Company discloses transverse transitions of an electrically conductive lattice structure implemented on a selective surface of glass. The patent states by measurements that when the polarization of the incoming wave is parallel to the lattice structure strips, the attenuation is significant, while the polarization is orthogonal to the strip direction, the transmission is more efficient. In the case of metallic venetian blinds, this means severe interference in the transmission of horizontal polarization when the metallic venetian blinds are oriented horizontally.
In addition to transmitting wave attenuation, metal strips can significantly interfere with the frequency selective surface applied to the selective film. The proximity of the metal strips can interfere with the function of the frequency-selective surfaces 20 in at least two ways. The first disturbance to the surface function is due to the near-field loading caused by the adjacent metal. This means that the metal parts of the metal venetian blinds are uncontrollably coupled to the filter elements of the frequency selective surface and unwantedly tuned to their operating frequency and transmission impedance. Another interference with the operation of the frequency-selective surface is due to unwanted reflections of the uncontrolled metal strip. In other words, part of the signal from the electromagnetic wave is reflected from the metal parts of the metal venetian blinds back into its upstream direction.
Figures 7a, 7b and 7c show slit radiators 207 formed by a slit beam aperture 201 transmitting a radio signal through an aperture 201 according to a preferred embodiment of the present invention, 220 through at least partially vertical polarization.
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The electrically conductive lattice structure 220 comprises a plurality of, preferably horizontal, electrically conductive strips 216 disposed at an angle 217 adjacent to the present low ejection surface 103. The orientation 217 of the electrically conductive strip 216 defines the projection 218 of the grid structure of the electrically conductive strip 5 on the low-emitting surface. Correspondingly, the orientation 217 of the electrically conductive strip 216 also defines the projection 219 of the grid structure on the low emptying surface of the non-conductive regions.
In a preferred embodiment of the slit radiator 207 of the radio transmitting aperture 1020 of the present invention, the narrow linear opening 203 is arranged to provide an incoming plane 301 from electric field vector 308 with a first positive charge distribution 208 and a first negative charge distribution 209 the electric motor force 204 acts on the boundary curve of the narrow linear opening 203 in the non-conductive region and wherein the electric motor force 204 is arranged at least partially vertical.
The arrangement according to a preferred embodiment of the gap radiator 207 disclosed herein further comprises a slidable aperture 205 formed by a narrow linear opening 203, and a current loop 210 circulating said shorted end 205. at least partially vertically polarized. The present narrow linear opening 25 203 also comprises a second short-circuit end 205 and a second current loop 210 circulating therethrough.
At least partially vertically polarized slit radiator 207, as disclosed herein, enables the transmission of a wireless signal through a window comprising metallic slats. The metal venetian blinds comprise a plurality of metal strips oriented horizontally, but there is no electrically conductive metal contact between them. A current loop 210 circulating a short-circuit end 205 of a narrow linear opening 203 as shown herein comprises a current maximum having a vertical flow direction. Any current flowing in the conductor couples the surrounding conductors with an opposite current, but in this case, a vertically oriented current loop 210
20185840 prh 08 -10-2018 does not connect reverse electrical current to the metal strips of the metal venetian blinds because the vertical current path between the venetian blind metal strips is interrupted.
At least partially vertically polarized slit radiator 207, as shown herein, is arranged to provide an electromotive force 204 that is at least partially vertically oriented. This electromotive force does not connect a uniform surface current mat in the direction of the electric field to the metal strips of the metal blinds, because the vertical current path between the metal strips of the blinds is interrupted.
At least partially vertically polarized slit radiator 207, as disclosed herein, allows the reception and re-radiation of electromagnetic energy through an insulating glass 15 through an aperture 201 transmitting a radio signal when the insulating glass element 100 is provided in a window comprising metal blinds.
An embodiment such as a preferred embodiment of the present invention comprises an insulating glass element 100 in which the radio-transmissive aperture 20 201 is provided on a first low-emptivity surface 103, and a second low-emptivity surface 103 provided with a conductive strips 216. The first and second low-emptiness surface 103 may be arranged in the same insulating glass element 100. The first and second low-emptiness surface 103 may also be arranged in the same window, each of which is arranged in a separate frame.
Method and Arrangement for Reducing Losses of Conductivity in a Low Ejection Surface by Undoing Differential Current Elements
According to an advantageous embodiment of the present invention, said reverse radiation efficiency attenuation is canceled
20185840 prh 08 -10-2018 currents, whereby individual narrow openings 203 become more efficient radiators. The method of the present invention can be applied to narrow apertures, wherein the apertures are preferably less than 200 µm wide, and wherein the individual apertures are arranged at least partially overlapping with one another. The method may also be applied to portions of the individual apertures 203, wherein the differential currents of the individual aperture mutually cancel the aperture in at least some portions of the aperture 203 comprising the focused radiation sources 303 of the gap radiator array 202. The method attenuates the relationship between the amplitudes of the differential currents and the amplitudes of common currents by portions of the edge curves of the slot-like opening 203, wherein said currents are centered on a closed envelope region 224 defining a bandwidth 103 defining the slot group
The present method is characterized in that the mutually reversing effect of the differential current elements occurs in the same conductor surface area, without substantially separating said currents between the non-conductive region. Thus, said currents are summed in the region of a single conductor such that residual reverse current elements of said current elements, vir20, provide electricity by non-conductive opening, separated from said current elements. By way of example, three adjacent electrical conductor regions can be mentioned, separated by two openings. In the sections of said openings, opposing current elements may flow on both sides of both openings. Specifically, the edges of the two openings between the three conductor surfaces can pass through four openings in the direction of the opening edge, of which in the middle conductor the two opposite current openings are summed and mutually canceled.
The present invention compensates for the loss of efficiency typically caused by low conductivity low surface area 30 surface loss by increasing the throughput signal efficiency on a coherent wavefront formed by a plurality of focused gap radiators, wherein at least one of the three spaced partially overlapping portions of openings 203 forming differential current elements. Said asymmetric
The distribution of 20185840 prh 08 -10-2018 may include widths of less than 5 mm and distances spaced more than 10 mm.
The arrangement according to a preferred embodiment of the present invention comprises a plurality of narrow linear openings 203 arranged in close proximity such that currents flowing at the edges of said openings interact with each other so that the summing and partial reversal of said currents enhance the operation of the performance.
Fig. 8a shows a slit radiator array 202 such as one of the preferred embodiments of the present invention, which exemplifies three separate narrow linear apertures 203 ', 203 "and 203'" in the low emptying surface 103, of which aperture 203 "is located in the middle.
In the example of Figure 8a, the electric field vector 308 of the incoming planar wave 301 induces electromotive forces 204 in apertures 203 on the low ejection surface 103 provided on the surface of the dielectric material, wherein the These currents are shown by means of current loops 210, and differential current elements 232 and 233 for refinement, wherein said differential current elements represent opposed currents flowing in the direction of the opening portion 25 at opposite edges of the opening. Current element 233 may be interpreted as a reverse current relative to current element 232.
An arrangement according to a preferred embodiment of the present invention comprises arranging portions of closely spaced narrow linear openings 203, at least in part, so that the differential current elements comprised by adjacent openings cancel each other out. This provides a significant improvement in the efficiency of the narrow linear opening as a slot emitter when applied to a low emitting surface such as a selective56
20185840 prh 08 -10- 2018 metal oxide surface of glass. Said overlapping opening portions may advantageously comprise single opening portions arranged to overlap with one another by arranging the opening edge curve. Said overlapping opening portions may also advantageously comprise separate opening portions 5 arranged in an overlapping manner as shown.
Said differential current elements do not function efficiently as sources of radiation because they flow in opposite directions at opposite edges of a single narrow opening and thus do not reinforce each other. However, said differential currents 10 effectively convert the electromagnetic radiation received in the gap emitter 207 provided on the low-emitting surface into heat by conductive losses. The conductivity of coatings used on glass surfaces is typically clearly weaker than, for example, copper, whereby resistive losses can be considerable.
When an electromagnetic wave encounters an aperture 203 formed on an electrically conductive surface, and thus forms a new radiation source, the interface between the incoming wave and the electrically conductive low-emitting surface 103 exhibits impedance mismatch reflection, the
The real part of said surface impedance comprises the radiation resistance due to the radiation loss formed by the gap radiator and the ohmic resistance due to the non-ideal electrical conductivity of the conductor surface. Said radiation resistance describes the desired electromagnetic energy that has ended up to be re-irradiated, while said ohmic loss resistance reduces the efficiency of the structure by converting the electromagnetic energy into heat at a low-emission surface.
In an arrangement according to a preferred embodiment of the present invention, the portions of the openings 203 are arranged in close proximity such that the differential current elements formed in the regions of the adjacent portions cancel each other so that the real impedance of the surface impedance on the low emitter surface 103
20185840 prh 08 -10- 2018 nose. In this way, the efficiency of the gap radiators formed in the non-ideal electrical conductor can be enhanced with respect to the gap radiators located far apart.
An arrangement according to a preferred embodiment of the present invention comprises arranging at least partially overlapping portions of closely spaced narrow linear openings 203 such that the differential current elements of adjacent openings cancel each other out and thereby reduce resistive losses in the low-emitting surface.
In the example of Figure 8a, a portion of the currents of the resonating current loop described above at the opening 203 'is described by the differential current elements 232' and 233 '. Similarly, the resonating current loop of the middle described opening 203 "is herein described by the differential current elements 232" and 233 "and the circulating current loop 210 of the short-circuit end 205 of the opening, and the resonating current loop of the lowest described opening 203 '" '' And 233 '' and opening by a short-circuited current 210. The openings 203 ', 203 "and 203'" may advantageously be arranged in close proximity so that the mutually acting effect of the differential current elements 20 is enhanced. As an exemplary, but not exclusive, mention may be made of a slit radiator array resonating in the 900 MHz bandwidth, wherein the spacing 234 of the opposite differential current elements 232 and 233 flowing and mutually flowing at the edges of two adjacent openings 203 is preferably of less than 30mm tenth. At distances of less than 10 mm, the currents in the opposite direction begin to effectively cancel each other out. When the differential current elements 234 are less than 5mm apart, the opposing current elements 30 232 and 233 within the region 231 delimited by the overlapping portions of the opening 203 overlap each other, and the surface current in the direction of the current current 210 is amplified in said conductive regions.
In the example of Figure 8a, the currents formed at the edges of the openings 203 ', 203 "and 203" are not similar to each other due to the combined effect of mutually canceling currents. Upper opening 203 'of differential current elements
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232 'has a stronger amplitude than current element 233' because opening element 203 "current element 232" cancels some of said surface current. Correspondingly, the lowest opening 203 '' of the differential current elements 233 '' has a stronger amplitude than the current element 232 ''. The differential current elements 232 "and 233" of the central opening 203 "5 do not form as intense an imbalance as the peripheral openings, but are each amplitude diminished to the outermost current elements of the outermost openings and to the common loop oscillating current loop 210.
The above arrangement causes narrow, linear apertures or portions of apertures in close proximity, preferably less than a tenth of a wavelength apart and overlapping with each other, to form a group within which the differential currents overlap each other, but reinforce each other because said current loops hate coherently, i.e. in the same phase and in the same direction. In the example of Fig. 8a, the current loops 210 rotating the short-circuited end of the opening form a common-mode current pattern, where the currents 210 of the individual openings arranged in close proximity to each other form a single current pattern. In the arrangement described, the currents circulating the short-circuited ends of the plurality of overlapping openings form a current pattern closely resembling a wide open orbit. By way of example, a wide opening may be mentioned as being about 2 to 5 cm wide.
The present invention compensates for the loss of efficiency typically due to low conductivity low surface area loss by increasing the throughput signal efficiency on a coherent wavefront formed by a plurality of focused gap emitters, wherein the transitions between partially overlapping portions of differential current elements forming portions of openings 203 in which said differential current elements cancel each other out. Said asymmetric spacing may include widths arranged to be less than 5 mm, as well as distances arranged to be more than 10 mm. Figure 8c shows a structure according to a preferred embodiment of the present invention, wherein:
20185840 prh 08 -10-2018, said openings 203 are partially overlapped and the spacing 234 of opposite differential current elements comprised by said openings is arranged asymmetric. Fig. 8b also shows a structure according to the present invention also with a symmetrical aperture spacing, wherein said apertures reflect wide slot radiators. Figure 8c illustrates an embodiment in which the radiation properties of narrow apertures are favorably affected by the present method, wherein the function of grouped narrow apertures as a gap emitter approximates that of apertures realized as wide apertures.
The current loops 210 depicted in Fig. 8c are formed by the sum of the current loops circulating the individual openings 203, where opposite differential current elements formed between adjacent openings 203 cancel each other out, and the currents circulating the shorted ends 205 of the openings 203 are summed. The electric motive forces 204 generated in the non-conductive areas of the individual openings 203 are summed in the same phase.
In the example of Fig. 8c, adjacent openings 203 are separated by uniform electrically conductive areas of low ejection surface 103 wherein the spacing 234 'of mutually canceling differential current elements is preferably less than 5mm. Opposite differential current elements formed in these common conductor regions weaken each other so that the permeability properties of the openings 203, which are in the form of a closely spaced gap radiator array, are significantly enhanced with respect to the spaced openings. In the example of Fig. 8c, the overlapping openings 203 are further separated by uniform electrically conductive areas of low emissivity surface 103 in which the spacing 234 'of the mutually canceling differential current elements is arranged to be multiplied by the spacing 234'. The arrangement described herein has created separate clusters of gap radiators in which said concentra- tions act as an effective gap radiator alone, and in which the summing of the waveguides 30 of said individual clusters increases the gain shown in the radiation pattern of the Building Supply 110 of the present invention.
The construction article 110 according to a preferred embodiment of the present invention comprises at least one electrically conductive low-emptying surface 103 provided with at least one opening 203 of an electromagnetic
20185840 prh 08 -10-2018 to enhance signal flow through a building material and having an opening having a conductivity substantially lower than a low-emptying surface 103, and wherein said at least one opening 203 comprises at least two opening portions separated by an electrically conductive region 231 there are two or more linear apertures, and that the distance 234 'between said portions, separated by said electrically conductive region 231 of the low-ejection surface 103, is many times the distance 234' between said linear apertures of said portion.
Electrical loading of low-level opening
An embodiment of a preferred embodiment of the present invention comprises a narrow linear aperture 203 provided on the low level surface 103, wherein said aperture 203 is arranged to function as a slot emitter 207 at a wavelength of oscillation. Said gap radiator further comprises at least a first loading area 403 and a second loading area 404 between which said opening 203 of the low conductivity surface 103 is arranged to form at least one non-conductive discontinuity point. Of said load areas
In accordance with a preferred embodiment of the present invention, gap impedance 405 between 403 and 404 may be loaded with impedance 405. Such impedance 405 may be provided, for example, by arranging said gap radiator to operate at new frequencies or impinging on some frequencies. Further, the impedance of said gap radiator can be adapted to the free space impedance more efficiently or in new frequency ranges.
Further, the impedances of the individual concentrated radiation sources 303 of the gap emitting surface 103 comprised of the low emitting surface 103 may be adjusted to rotate the radiation beam formed by said gap emitter group at some operating frequency 30. Said load impedance 405 can be implemented by any control element. Typical control elements are e.g. passive coils, resistors, capacitors, or phase shifters, each of which may be implemented with either discrete components or longitudinal components, or with a short or long transmission line portion. The control elements may also include active or actively adjustable load elements, such as transistors or varactors.
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Figures 9a and 9b show slit radiators according to some preferred embodiments of the present invention in which passive longitudinally distributed components are provided in the discontinuity regions between the load areas 403 and 404.
Fig. 9a shows an arrangement in which a longitudinally distributed inductance is provided in the area of the low ejection surface 103 between said load areas 403 and 404, wherein said inductance is coupled between two portions of an edge curve of a breast opening 203. Said longitudinally distributed inductance 10 can be arranged, for example, such that a portion of the curve of the opening 203 is curved. Said inductance is arranged in the electrically conductive region 23T of the low emptying surface 103 in Fig. 9a. The parameters of said inductance depend on the geometry of the arrangement and the properties of the materials used. For example, the inductance 15 formed on the selective surface of the glass also comprises a series resistor which can be remarkably high when compared to, for example, a similar geometry formed on an aluminum surface. Said inductance forms a filter structure arranged in parallel with opening 203. Said filter structure generates a frequency-dependent load impedance at the gap radiator 207, wherein said load impedance is coupled in parallel with said gap radiator. Said load impedance may comprise, for example, a high impedance approaching an open-circuit load, whereby the surface current formed on the low-emitting surface 103 does not substantially flow through that impedance at the frequency at which the high impedance is provided.
Fig. 9b shows an arrangement for generating a new resonant frequency of a gap radiator in which a longitudinally distributed inductance is provided in the area of low dissipation surface 103 between the load regions 403 and 404, and capacitance connected in series with said inductance to form a resonance. Said resonant circuit forms a filter structure arranged in parallel with the opening 203 and the loading areas 403 and 404. Said inductance is arranged in the electrically conductive region 23T of the low ejection surface 103 in Fig. 9b. Said capacitance forming the resonant circuit is shown in Fig. 9b for a portion of the opening 203 between the conductive region 231 'and the load region 404.
Said resonant circuit generates a frequency-dependent load impedance
20185840 prh 08 -10-2018 to a gap radiator 207, wherein said load impedance is coupled in parallel with said gap radiator.
A band-pass, band-pass, high-pass or low-pass filter may also be arranged between two separate gap radiators, whereby separate gap radiators 207 formed by openings 203 may be combined to create new resonant bands.
Fig. 10a illustrates an embodiment of a preferred embodiment 10 of the present invention wherein the building material 110 comprises a dielectric material 229 and a low-emptying surface 103, wherein said low-emitting surface is provided with an opening 203 the transmission characteristics 15 are controlled by a load impedance 405. Said load impedance is in communication with the interface element 402, which in this example is implemented by an electrically conductive strip. Said connection element can be implemented either by galvanic contact or by an arrangement operating only through an electric or magnetic field. In the example of Fig. 10a, said interface element is implemented by capacitive coupling.
The interface element 402 of Fig. 10a provides an electrical connection between the oscillating surface currents and electric fields in the low-emitting surface area 103 of the gap radiator and the load impedance 405 that controls them. Said low-emission 25 vitite surface 103 comprises an opening 203 arranged as a gap radiator and provided with at least a first loading area 403 and a second loading area 404 between which said opening 203 is arranged to form at least one electrically non-conducting discontinuity. The gap radiator 207 between said load areas 403 and 404 can now be loaded with an impedance 405 in various frequency ranges according to a preferred embodiment of the present invention.
Fig. 10b illustrates a structure according to a preferred embodiment of the present invention, wherein the building material 110 comprises at least 35 dielectric material 229 and a low emitter surface 103 and a radio signal from a gap emitter 207 disposed on said low emittance surface 103.
20185840 prh 08 -10-2018 to form a permeable aperture. The arrangement further comprises an interface element 402 and a matching component 407. Said matching component 407 may comprise either discrete components or longitudinal distributed matching components, or a phase shifter such as a short transmission line. The mating components mentioned in Example 5b of Figure 10b as well as said interface element are implemented on a circuit board 406 where the circuit board further provides a mechanical fastening. Said circuit board may be implemented, for example, as a flexible circuit board, or as a flexible circuit board, and may also comprise mechanical components, for example for mounting. The interface element 402 or the adapter component 406 can also be implemented without a separate circuit board. These can also be applied directly to the surface of said dielectric material 229, for example, by printing, printing, or any other additive method.
Said matching component may comprise either discrete components or longitudinal distributed matching components. The adapter components mentioned in the example of Fig. 10b, as well as said interface element, are implemented on a circuit board 406 where the circuit board further provides mechanical fastening. Said circuit board may be implemented, for example, as a flexible circuit board, or as a non-flexible one, and may also comprise mechanical components, for example for mounting. The interface element 402 or the adapter component 406 can also be implemented without a separate circuit board. These can also be applied directly to the surface of said dielectric material 229, for example, by printing, printing, or any other additive method.
Fig. 10c illustrates a structure according to a preferred embodiment of the present invention, wherein the building material 110 comprises at least a transmissive transducer 30 of dielectric material 229 and a first low-emptivity surface 103 arranged on its first surface and a gap emitter 207 disposed on said first low-emission surface 103. The arrangement further comprises a second low-emissivity surface 103 disposed on one of the surfaces of said dielectric material 229 and a gap-emitting aperture arranged on the second low-emissivity surface 103 to form a radio-transmitting aperture. The arrangement further comprises an interface element 402, and an adapter component 407 arranged in connection with the low low activity surfaces of the mo35. The arrangement illustrated in the example of Fig. 10c may be implemented, for example, in an insulating glass element
20185840 prh 08 -10- 2018
100 connections, which may comprise multiple low ejection surfaces. The arrangement described provides a load impedance, the circuit board 406 of which can be implemented, either partially or completely, with the gases of the insulating glass element, or outside the glass elements. Said circuit board 406 may be implemented as either a flexible tape or a solid structure.
Fig. 10d illustrates a structure according to a preferred embodiment of the present invention, wherein the building material 110 comprises at least a radio transmitting signal transducing through a gap emitter 207 of at least dielectric material 229 and a first low emitting surface 103 provided on its first surface. The arrangement further comprises a second low-emissivity surface 103 disposed on one of the surfaces of said dielectric material 229, and a radio-transmissive aperture 15 arranged on the second low-emissivity surface 103. The arrangement further comprises an interface element 402 and an adapter component 407 arranged in association with both low-ejection surface surfaces. The arrangement illustrated in the example of Fig. 10d may be implemented, for example, in connection with an aluminum-faced insulating board, which may comprise a plurality of low-emptying surfaces. The Ku20 arrangement provides a load impedance implemented by the circuit board
The 406 may be positioned on either side of the low ejection surface 103. Said circuit board 406 can be implemented as either a flexible tape or a solid structure. The circuit board comprising the adapter components and the connection element in the form of a tape or a film may further form a vapor barrier.
Adjusting Low Permeability Permeability Properties
The transmission characteristics of the aperture transmitting the radio signal may be adjusted by adjusting the properties of the gap radiators of the gap radiator array comprising said aperture by means of a related load impedance 405. Said load impedance 405 communicates with an interface element 402, wherein said interface element forms an electromagnetic coupling with the first and second loading areas of the low-discharge surface. Said electromagnetic coupling can be implemented as a galvanic, inductive or capacitive coupling.
20185840 prh 08 -10- 2018
Fig. 11a shows a building accessory 110 according to a preferred embodiment of the present invention, comprising at least a dielectric material 229, and a low emptying surface 103 disposed thereon, wherein a plurality of openings 203 are provided to increase the electromagnetic signal flow through the building material; the radio-transmitting aperture comprises a group of gap radiators 207 formed by slit radiators 207, wherein the shortest dimension of said radio-transmitting aperture is preferably arranged to be less than a wavelength by means of a slit Said dimension 305 may advantageously be arranged in the width of the aperture in the horizontal direction. Said openings 203 comprise meandering edge curves in which the arcuate openings are arranged partially overlapping with each other.
11a further illustrates a control unit 408, wherein said control unit 408 communicates with a matching component 407 implementing said load impedance 405. and the control unit 408 can only be used to control the load impedances 405, wherein said control unit 408 is only involved in adjusting the characteristics of the signal passing through the low-emptying surface 103. Said adjusting of the features comprises at least adjusting the low impedance surface penetration impedance, the frequency response, the beam forming and the effects of acting as a filter.
An embodiment of a preferred embodiment 30 of the Building Material 110 of the present invention comprises at least two gap radiators 207 which are loaded with different load impedances 405, wherein said gap radiators 207 are provided either as part of a single opening 203 or as separate openings 203.
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The load impedance illustrated in Fig. 11a is in communication with an interface element 402 'and 402', wherein said interface elements communicate with the load areas 403 and 404 arranged on the low-emptivity surface 103, and with the arrangement forming the load impedance 405. Said connection elements can be implemented either by galvanic contact or only by an arrangement operating through an electric or magnetic field, such as a capacitive plate or strip, or an inductive loop.
The control unit 408 according to a preferred embodiment of the Building Material 110 of the present invention comprises an arrangement for adjusting the load impedance 405. In addition, said control unit 408 may be arranged to establish a wireless connection 409 to another wireless device. Said connections may be provided, for example, to base stations outside the building, to base stations inside the building, to wireless communication devices inside or outside the building.
401, etc. The said control unit may be provided such that a single unit controls a plurality of load impedances, or such that a single control unit controls a single load impedance.
The control unit 408 according to a preferred embodiment of the Building Supply 110 of the present invention may perform modulation, demodulation and amplification of the wireless signal. It can also perform frequency aggregation and carrier aggregation. Said control unit 408 may be arranged to transmit information between two communication links using different network techniques or protocols. For example, said control unit 408 may be arranged to transmit information between WLAN or WiGig networks and wireless mobile communications (such as 2G, 3G, 4G, LTE-advanced, 5G, or their evolution).
The control unit 408 according to a preferred embodiment of the Building Supply 110 of the present invention may comprise a microcontroller, a power supply, electronic memory areas, or external interfaces such as a usb port.
The control unit 408 according to a preferred embodiment 35 of the Building Material 110 of the present invention may be provided with a fixed extension67
20185840 prh 08 -10-2018 for establishing a connection 410, wherein said control unit 408 is provided as part of a building communications connection such as a local area network or fiber optic cable. In such a case, the building's internal signaling may be based on a conventional fiber-optic network, but the connection outside the building may be implemented through wireless connections.
By providing an extension connection 410 to the fiber network of the building, a separate control unit 408 can be installed in the building to control the electromagnetic signal transmission characteristics of the building components 110 of the present invention housed in individual room wall structures. This method can be utilized, for example, for the benefit of base station network load and resource allocation, whereby sources of interference can be filtered, or carriers are controlled for the benefit of conditions requiring the highest re15 resources. Said separate control unit 408 may communicate with the base station network backbone network via an extension connection 410, or it may establish a wireless connection 409 with base stations.
The control unit 408 according to a preferred embodiment of the Building Material 110 of the present invention comprises an arrangement for adjusting the transmission characteristics of the radio-transmitting aperture 201 and the radiation pattern formed by the gap radiator array 202 comprising said aperture at one or more frequencies.
The control unit 408 according to a preferred embodiment of the Building Material 110 of the present invention comprises an arrangement for adjusting the impedance of the gap radiator 207 at one or more frequencies comprising a radio-transmitting aperture 201. Said impedance control may be used to adjust the radiation pattern formed by the gap radiator array 30 202 of said aperture 201.
Fig. 11b illustrates an arrangement according to a preferred embodiment of the Building Material 110 of the present invention, comprising a load impedance 405 arranged in connection with a gap radiator for adjusting the low-emission 35 surface penetration characteristics. The building material 110 may comprise either one or more low-emptiness surfaces, where mentioned
20185840 prh 08 -10-2018 load impedances 405 are provided to control the impedances of the gap radiators. Fig. 11b shows an arrangement in which the aperture 201 formed in the building material 110 is arranged to receive plane waves 301 'and 301 "and to re-emit plane waves 304' and 304 to the opposite side of building material 5 110, where plane waves 304 'and 304 wave fronts propagating in polarizations.
Fig. 11c shows an arrangement according to a preferred embodiment of the present invention. Said arrangement comprises a building material 110 having an aperture 201 for receiving plane waves 301 'and 301 "and for re-emitting plane waves 304' and 304" on the opposite side of a building material 110, wherein said aperture comprises for adjusting low penetration surface penetration properties. Said load impedance 405 is arranged to prevent the plane wave 301 'from passing through said aperture 201, wherein said wave 301' forms a reflected reflective wave front 306. The incoming wave 301 ', whose transmission according to the present invention is attenuated, may comprise either an interference signal a signal oscillating at a different frequency.
Fig. 11d shows an arrangement according to a preferred embodiment of the building material assembly 110 of the present invention, wherein the radiation pattern formed by the slit radiator group comprising the radio-transmitting aperture 201 is controlled by at least one side of the slit radiator group 40 Said radiation pattern control may be performed at one or more operating frequencies comprised by the gap radiator.
Said radiation pattern control can also be implemented at a frequency different from the operating frequency of the gap radiator array, such as the frequency of an interference signal. The plane wave 301 'depicted in Fig. 11d may comprise, for example, its signal propagating at a frequency different from the frequency of the wave 301'. For example, the present arrangement may be advantageous in cities where base stations are located on the roofs of buildings. Said wave 301 '
20185840 prh 08 -10-2018 may also comprise, for example, a signal transmitted by an interference generating device inside the building, the direction of which is to be blocked to the base station to eliminate the interference.
Fig. 11e shows an arrangement according to a preferred embodiment of the Building Material 110 of the present invention, having at least one low-emitting surface 103 provided with an opening 203 for forming a radio-transmissive aperture 201, said aperture 201 comprising a load impedance a portion of the incoming electromagnetic signal energy to a control unit 408 arranged in connection with the Building Material 110, wherein the control unit may preferably comprise at least a radio frequency transceiver or a wireless sensor. Said load impedance 405 may be used to convert some opening 203 of said building accessory 110 comprising a low release sidewall surface 103 into an antenna such that said load impedance 405 comprises at least a matching circuit or transmission line disposed between a control unit 408 and a low landing surface 103. Said matching circuit may comprise a structure forming either capacitance or inductance, or it may be an actively adjustable matching component. Said antenna may be used to establish a wireless connection 409.
A building accessory 110 according to a preferred embodiment of the present invention comprises at least one opening 203 arranged to form a gap radiator array 202, wherein said gap radiator array 202 is arranged to act as an antenna array by at least one load impedance 405, wherein said load impedance Between the control unit arranged in connection with the building material. Said antenna array may also comprise a plurality of load impedances, at least some of which are arranged to adjust the radiation pattern or operating frequencies of the antenna array. Said antenna array may comprise multiple operating frequencies and multiple polarizations.
20185840 prh 08 -10- 2018
The building material 110 may comprise either one or more low-emplacement surfaces, wherein said load impedances 405 are arranged to control the impedances of the gap radiators. Fig. 11e shows an arrangement in which the aperture 201 formed in the building material 110 is arranged to receive plane waves 301 'and 301 "and to re-emit plane waves 304' and 304 to the opposite side of building material 110, where plane waves 304 'and 304 wave fronts propagating in different polarizations.
Figures 11a-11e show an arrangement according to a preferred embodiment of the Building Material 110 of the present invention, wherein the Building Material is a window. Said window comprises at least a first dielectric material 229, wherein said dielectric material is glass, and a low-emissivity surface 15 103 arranged on said dielectric material, wherein said low-emissivity surface 103 is a selective surface, anti-fog surface, sunscreen surface, semiconductor surface. Said window further comprises an insulating glass element comprising at least a first and second glass sheet, wherein at least one glass sheet comprises said dielectric material 229, and a sealed space 105 of air 20 disposed between said glass sheets. Said building material may further comprise a printed circuit board 406 forming a load impedance 405. the load impedance 405 may be coupled to a window frame structure or wall structure, for example, by means of a transmission line such as a cable or twin wire, wherein said frame structure or wall structure may be coupled to 25 control units 408 which may be coupled to a further connection 410. building material 110. Said building may comprise a plurality of building materials according to the present invention which constitute either a wireless a connection 409, or an extension 410 otherwise provided, wherein said extension may be provided from a building to a base station, a backbone network, or some wireless communication device 401.
Figures 11a-11e illustrate an arrangement according to a preferred embodiment of a building article 35 of the present invention 35 where
20185840 prh 08 -10- 2018 the building accessory is a thermal insulation board. Said insulating board comprises at least a first dielectric material 229, wherein said dielectric material has a density of less than 200 kg / m 3. Said dielectric material may be, for example, PIR, PUR or EPS material, or some other heat insulating material. The dielectric material may also be a thin film. Said film may be laminated into a part of a low-emptying surface, for example a vapor barrier, or it may be arranged, for example, in a vacuum-producing closed chamber. Said insulating sheet further comprises a low-emitting surface 103 arranged on the surface of said dielectric material, wherein said low-emitting surface 10 is aluminum. Said building material may further comprise at least a partial vapor barrier arrangement in which the vapor barrier is implemented with either a film or tape, which may comprise a printed circuit board 406 forming a load impedance 405 and a matching component 407. said control unit may be connected to a plurality of separate building materials 110 of the present invention. Said building may comprise a plurality of building materials according to the present invention that form either a wireless connection 409 or otherwise arranged 410. , wherein said extension may be provided from the building to the base station, the backbone, or some wireless communication device 401.
In a method according to a preferred embodiment of the invention, signal propagation through a building material 110 comprising at least one electrically conductive low surface surface 103 is provided, wherein the method comprises forming an opening 203 having a lower electrical conductivity forming at least one closed edge curve 223, wherein said opening 203 defines a closed envelope 224 such that said opening 203 is within the closed envelope 224 and has an area substantially greater than the area of the inner opening of the closed envelope 223 and closed by the closed envelope 224 length substantially less than the length of 35 closed edge curve 223 to form at least one internal matrix of area defined by closed curve 224 alaemissiviteettipinnan
20185840 prh 08 -10- 2018
103 region 231, at which closed envelope 224 does not coincide with edge curve 223.
In a method according to a preferred embodiment of the invention, the closed edge curve 223 of the opening 203 is formed to coincide with the closed edge curve 227 delimiting the low ejection surface 103.
In a method according to a preferred embodiment of the invention, the closed edge curve 223 of the opening 203 forms a closed edge curve separated from the closed edge curve 227 delimiting the low surface area 10 103.
In a method according to a preferred embodiment of the invention, said aperture 203 generates at least one positive distribution 208 and negative 15 209 charge distribution acting as poles of the surface current formed on the low emptying surface 103 by a first polarization which, together with said surface current formed on the low-emitting surface 103, forms a reso20 nance circuit for generating a gap radiator 207 acting as a concentrated radiation source 303 through a building material to enhance the propagation of the electromagnetic signal through the building material.
In a method according to a preferred embodiment of the invention, the spreading surface 103 of the mata25 is provided with a gap radiator array 202 comprising at least two of said gap radiators 207 to form an aperture 201 transmitting radio signals, wherein said radius defines in the building material 110 an area delimited by a closed curve 230 wherein said radio-transmitting aperture 201 is within said closed curve 230 and having a surface area defined by a closed curve 230 substantially smaller than a closed edge area 227 delimiting a low-emptying surface 103.
20185840 prh 08 -10- 2018
In a method according to a preferred embodiment of the invention, said radio-transmitting aperture 201 is formed to be less than one wavelength in width and at least one wavelength in height to the lowest of said slit radiators 207 of the slit radiator array 202 comprising the aperture 201.
In a method according to a preferred embodiment of the invention, a low emitting surface 103 is provided with a gap emitter group 202 comprising at least two of said gap emitters 207, wherein said focused emitters 303 207 at the lowest resonant frequency, and wherein said vertical array may be straight or twisted.
In a method according to a preferred embodiment of the invention, said aperture 203 generates at least one positive 208 and negative 20 209 charge distribution acting as poles of a surface current formed on a low emptying surface 103 by a second electromagnetic which, together with said surface current formed on the low-emitting surface 103, forms a resonance circuit electr25 as a concentrated radiation source 303 which enhances the passage of the electromagnetic signal through the building material in a second polarization, with first and second polarization transitions.
In a method according to a preferred embodiment of the invention, the low ejection surface 103 is formed on the surface of the dielectric material.
In a method according to a preferred embodiment of the invention, the dielectric material is glass.
In a method according to a preferred embodiment of the invention, the dielectric material is used as dielectric material.

权利要求:
Claims (25)
[1]
A building material (110) comprising at least one electrically conductive low-emptying surface (103) provided with at least one opening (203)
[2]
2. claimed in claim 1 construction equipment (110), characterized in that the resonant circuit comprised in the resonant dimension of the slot radiator formed by the opening (203) (207) (215) is preferably arranged at the incoming side length of a plane wave (301) for frequency of vibration.
[3]
A building material (110) according to claim 1 or 2, characterized in that said at least one opening (203) is arranged to form an electric field, said at least partially overlapping edges being overlapping in the direction of the electric field acting over the edges.
[4]
Building material (110) according to claim 1, 2 or 3, characterized in that said at least one opening (203) comprises at least two opening portions separated by an electrically conductive region (231) of a low-emptying surface (103), said opening portions having two or more linear
25 openings, and that the distance (234 ') between said portions is several times the distance (234') between said linear openings of said portion.
[5]
Building material (110) according to one of Claims 1 to 14, characterized in that a band pass, band stop, high pass or low pass filter is provided between the two separate gap radiators (207) to combine the gap radiators (207) formed by separate openings (203). in order to create.
A building material (110) according to any one of claims 1 to 4, characterized in that said closed edge curve (223) of said at least one opening (203) or the closed edge curve (227) defining said low edge surface (103) comprises at least one portion arranged to meander.
5 and a second loading area (404) between which said opening (203) in the low conductivity area (103) is arranged to form at least one non-conductive discontinuity, and wherein said gap radiator (207) is loaded with impedance between said loading areas (403) and (404). 405).
5 to enhance the passage of the electromagnetic signal through the Building Supply, the opening of which has a substantially lower electrical conductivity (103), characterized in that:
- the edges of said at least one opening (203) disposed on the low ejection surface (103) form at least one closed edge
[6]
Building material (110) according to one of Claims 1 to 5, characterized in that at least two earthing surfaces (103) are provided on the low-surface side surface (103).
20185840 prh 08 -10-2018 a slit radiator array (202) comprising a slit radiator (207) for forming a radio-transmitting aperture (201), wherein said slit radiators (207) are arranged to form at least said first polarization electric fields (30) and said radio-transmitting aperture (201) defining for the building material (110) an area delimited by a closed curve (230), wherein said radio-transmitting aperture (201) is inside said closed curve (230) and having a surface area defined by a closed curve (230). is substantially smaller than the area delimited by the closed edge 10 curve (227) delimiting the low ejection surface (103).
[7]
A building material (110) according to claim 6, characterized in that said radio-transmitting aperture (201) has a width of less than one wavelength and a length of at least one wavelength.
[8]
A building material (110) according to any one of claims 1 to 7, characterized in that at least two positions are provided on the low-lying surface (103).
[9]
Building material (110) according to one of Claims 1 to 8, characterized in that said opening (203) is arranged to form at least one
A positive (208) and a negative (209) charge distribution of the surface current formed on the thalamic surface (103) as a result of an electromagnetic signal oscillating in a second polarization, an electromagnetic signal encountered by the building material (110), and in mentioned with a surface current (210 ") formed on a low deposition surface (103)
20185840 prh 08 -10-2018 provides a resonant circuit for generating a gap radiator (207) operating in a second polarization as a concentrated radiation source (303 ”) through the Building Material, wherein the first and second polarizations are mutually intersecting.
[10]
10 (103), and that the low emitting surface (103) is either a selective surface, an antifreeze surface, a semiconductor surface, a self-cleaning surface, or a sunscreen surface.
Building material (110) according to one of claims 1 to 9, characterized in that said building material is an insulating glass element (100) comprising at least two glass sheets (102), an intermediate space (105) between them and at least one of which glass sheets (102) providing said low ejection surface
10 curves (223), and that
- the edges of said openings (203) define a closed envelope (224) such that said openings (203) are inside a closed envelope (224) and have an area substantially greater than the area of the closed envelope (224).
[11]
Building material (110) according to one of Claims 1 to 9, characterized in that the low ejection surface (103) is arranged on a surface of dielectric material, said dielectric material being an insulating material having a density of said insulating material of less than 200 kg / m3.
[12]
Building material (110) according to any one of claims 1 to 11, characterized in that said load impedance (405) is implemented by a control element, which control element is a passive coil, resistor, capacitor, or phase shifter implemented by either discrete components, longitudinally distributed components, or a short or long portion of the transmission line, or that said adjusting element includes active or actively adjustable load elements.
[13]
Building material (110) according to one of Claims 1 to 12, characterized in that a longitudinally distributed inductance is provided in the area of the low release surface (103) between said load areas (403) and (404).
30 a dance wherein said inductance is coupled between two portions of an edge curve of a breast opening (203).
[14]
Building material (110) according to one of Claims 1 to 13, characterized in that the low-lying strips between the load areas (403) and (404)
A resonant circuit is provided in the region of the dip (103) of the 20185840 prh 08 -10-2018 to form a new resonant frequency, said resonant circuit providing a frequency-dependent load impedance to the gap radiator (207).
[15]
15 openings (203), or as separate openings (203).
15 aperture (201) having a gap radiator array (202) at the lowest resonant frequency of said gap radiators (207).
The surface area and length of the inner openings (203) 15 (224) is substantially smaller than the length of the closed edge curve (223), thereby forming at least one electrically conductive region (231) of the low edge surface (103) enclosed by the closed envelope (224). envelope curve (224) not coinciding with edge curve (223)
[16]
A building material (110) according to any one of claims 1 to 15, characterized in that said building material (110) comprises at least two gap radiators (207) which are loaded with differing load impedances (405), wherein said gap radiators (207) are arranged
[17]
Building material (110) according to one of claims 1 to 16, characterized in that said building material (110) comprises a control unit (408) for adjusting the load impedance (405).
[18]
A building accessory (110) according to any one of claims 1 to 17, characterized in that at least one low ejection surface (103) of said building accessory (110) is provided with an opening (203) for forming a radio transmitting aperture (201). -
A load impedance (405) arranged in connection with 25 radiators (207) arranged to direct at least a portion of the energy of the incoming electromagnetic signal to a control unit (408) arranged in connection with a building material (110).
30
[19]
A building material (110) according to any one of claims 1 to 18, characterized in that said building material (110) comprises a control unit (408), the control unit (408) comprising an arrangement for adjusting one or more of the impedance of the gap radiator (207) on more frequencies.
20185840 prh 08 -10- 2018
[20]
A building material (110) according to any one of claims 1 to 19, characterized in that said impedance (405) is arranged to control the impedance of said gap radiator (207) or the radiation characteristics of said gap radiator array (202).
A plurality of slit radiators (207) comprising a plurality of slit radiators (202), wherein the focused radiation sources (303) comprising said slit radiators (207) are arranged in a vertical sequence, wherein said at least two adjacent, (207) a lower bar at a resonance frequency, and wherein said vertical string may be arranged straight or meandering.
20 with, and where
- said electrically conductive region (231) of the low ejection surface (103) defining at least two edges of the opening (203) arranged at least at a distance (234), wherein said edges are at least partially overlapping;
25 - said opening (203) is arranged to provide at least one positive (208) and negative (209) charge distribution of the surface current formed on the low-emitting surface (103) by a vibrating electromagnetic signal encountered in the first polarization of the building material (110); , an electric field vector oscillating in its first polarization between its two edges, which together with said surface current (210) formed on a low-emitting surface (103) forms a concentrated radiation source (303) that enhances the transmission of an electromagnetic signal from the resonant circuit
35 for forming a first gap polarizer (207),
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- said resonance circuit of said slit radiator (207) is resonant at at least one frequency between 300 MHz and 30 GHz, and
- said slit radiator (207) comprising at least a first loading area (403) arranged on said low level surface (103),
[21]
Building material (110) according to one of Claims 17 to 20, characterized in that said impedance (405) is connected to the control unit (408) either by capacitive, inductive or galvanic connection.
10
[22]
A building accessory (110) according to any one of claims 17 to 21, characterized in that said control unit (408) is arranged to establish a wireless connection (409) to a communication device separate from the building accessory.
15
[23]
A building accessory (110) according to any one of claims 17 to 22, characterized in that said control unit (408) is arranged to establish an extension connection (410) to a communication device separate from the building accessory.
[24]
A building material (110) according to any one of claims 1 to 23, characterized in that said opening (203) has an area of not more than one percent relative to the area of said low extraction surface (103).
A method for enhancing signal flow through a building material (110) comprising at least one electrically conductive low
[25]
25, wherein the method comprises forming an opening (203) with a lower conductivity surface (103) having a conductivity substantially lower than the low emissivity surface (103), characterized in that the edges of the at least one opening (203) provided in the method a closed edge curve 30 (223) such that the edges of said openings (203) define a closed curve (224) within which said opening (203) is formed and the area defined by the closed curve (224) is formed substantially larger than the closed curve (224) ), the area and length of the inner opening (203) being substantially smaller than the length of the closed edge curve (223) 35, thereby forming at least one electrically conductive region (231) of the low edge surface (103) enclosed by the closed envelope (224); 224) is not coincident with the edge curve (223), wherein said conductive region (231) of the low-emptying surface (103) defines at least two edges of the opening (203) disposed at least at a distance (234), wherein said edges are at least partially overlapping such that said opening (203) being arranged to provide at least one positive (208) and negative (209) charge distribution of polarized surface current (103) on the surface of the low current surface (103) due to an electromagnetic signal oscillating in the first polarization; an electric field vector oscillating in the first polarization between the two edges, which, together with said surface current (210) formed on the low-emitting surface (103), forms a resonant circuit as a concentrated radiation source (303) for enhancing electromagnetic signal propagation through the building material; a first radar (207), and wherein said resonance circuit of said gap radiator (207) is arranged to resonate at least one frequency between 300 MHz and 30 GHz, and wherein said gap radiator (207) comprises at least a first 403), and a second loading area (404) between which the opening (203) in the conductive region of the low surface line (203) is arranged to form at least one non-conductive discontinuity, and wherein a gap radiator (207) between said loading areas (403) and is loaded with impedance (405).

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FI127700B|2018-12-31|Building material

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FI12279U1|2019-02-15|Building material

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US20220085866A1|2022-03-17|A diversity scattering device and method for using the same

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FI128682B|2020-10-15|A diversity scattering device and method for using the same

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FI127591B|2018-09-28|Device and method for receiving and re-radiating electromagnetic signals

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同族专利:

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公开号 | 公开日

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EP3673137A2|2020-07-01|

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WO2019073116A3|2019-05-23|

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US20200321703A1|2020-10-08|

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US20210083375A1|2021-03-18|

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DK3673137T1|2020-10-12|

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US10879603B2|2020-12-29|

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EP3673137A4|2021-04-28|

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AU2018350236A1|2020-05-21|

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WO2019073116A2|2019-04-18|

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CA3078665A1|2019-04-18|

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法律状态:

优先权:

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申请号 | 申请日 | 专利标题

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FIU20174233U|FI12210U1|2017-10-10|2017-10-10|Insulating glass element|

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FIU20174243U|FI12277U1|2017-10-10|2017-10-27|Insulating glass element|

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FI20176043|2017-11-22|

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