Magnetic device and method for making the same

专利摘要:
The ferromagnetic changeover device consists of a wire section (10) in which a jacket part (12) and a core part (11) can be magnetised differently. The wire consists of an alloy of cobalt, vanadium and iron. The jacket part and the core part thus have either a matching state, with the same magnetisation direction of the core part and of the jacket part, or a reverse state, with a different magnetisation direction of the core part and of the jacket part. The coercive force of the core part (11) is sufficiently large for the magnetisation of the jacket part in the matching state not to be able to change the core part over into the reverse state. It is thus possible to change over from one state to the other only by means of an external magnetic field. This results in pulses of more than 1.5 V and with a width of 20 mu s being induced in the case of an external magnetic field having a positive half-cycle with a peak value of 11940 A/m and a negative half-cycle with a peak value of 1592 A/m in a coil having 925 turns on a wire section 10 with a length of 3 cm. The changeover device can be used for determining proximity, time measurement and coding. <IMAGE>
公开号:SU1041048A3
申请号:SU782617555
申请日:1978-05-03
公开日:1983-09-07
发明作者:Ричард Виеганд Джон
申请人:Дзе Эглин Мануфактуринг Компани (Фирма)；
IPC主号:

专利说明:

The invention relates to electrical engineering, more specifically to magnetic devices and methods for their manufacture. A magnetic device is known, made in the form of a homogeneous chemical composition of magnetic wires, having a shell and a heart of wine, and having the ability to magnetize in an external magnetic field along its axis and be in a state of coincidence when the direction of the shell and core parts decreases. coincide, and the opposite state - when they are opposite, and the coercive force of the shell part is greater than the coercive force of the core part and in the absence of an external magnetic field, the device a back reside only in state l. The disadvantages of the known device are relatively low sensitivity and non-optimal signal-to-noise characteristic. In order to increase the sensitivity of the bone and improve the signal-to-noise performance in a magnetic device, made in the form of a homogeneous chemical composition of the magnetic wire having sheath and core parts and having the ability to magnetize in an external magnetic field along its axis and be in a state of coincidence where the magnetization directions of the shell of the carpet and the core parts coincide, and the opposite state - when they are opposite, and the coercive force of the shell part is greater than the coercive force of the heart the other part, the core part is made so that it has a coercive force sufficient to maintain in the absence of an external magnetic field a state of coincidence, and the relative magnetic properties of the core and shell parts are chosen so that the device is switched from a reverse state to This doesn’t happen either by reversal of the core part by bistrae, than vice versa. A known method of manufacturing a magnetic device, which includes the operations of heat treatment, cyclic deformation crimping under the tension of the magnetic wire, and the deformation twist in both directions rc are produced to the same degree 2j. The disadvantage of this method is the relatively low sensitivity of the magnetic device obtained with it . In order to increase the sensitivity of the magnetic device in the method of manufacturing a magnetic device, which includes heat treatment operations, cyclic deformation torsion under the tension of the magnetic wire, deformation torsion in one direction is produced more than in the other. FIG. 1 is a schematic representation of a ferromagnetic wire in the reverse state, enlarged; in fig. 2 is a diagram of a solenoid excitation device used to create an external field, acting on a magnetic wire, and a receiving coil used to generate an output: signal in response to a change in the magnetic state of the wire to the opposite; in fig. 3 is a graphical depiction of an asymmetric type of magnetic reversal of a wire, obtained from the results of a test carried out using the device of FIG. f and it shows the exciting external field, hysteresis loop and the resulting output pulses; in fig. 4 - the same, symmetric type; in fig. 5 is a schematic representation of a mechanism for treating a magnetic wire according to the invention. , FIG. Figure 1 shows a variant of the magnetic wire 1 according to the invention, consisting of a material containing cobalt, iron and vanadium. A piece of magnetic wire has a circular cross section, preferably exactly circular or close to an exact circle of cross section5 | . The most suitable pieces of wire with a diameter of about 0.25 mm and a length of 1-3 cm. The wire is processed to obtain a single magnetic wire element 1 having a relatively core part 2 with a relatively low coercive force and a relatively rigid sheath part 3 having a relatively high coercive force . With respect to the soft core part 2 (Fig. 1), magnetic anisle Yudn-M, the axis of easy magnetization running parallel to the axis of the wire. The relatively rigid shell part 3 is also magnetically anisotropic, with the axis of the magnetization coherence providing the resultant magnetization parallel to the axis of the wire. The direction of magnetization of the core part 2 f depends to a large extent on the effect of the magnetic field of the shell part and on any external magnetic field. In the shown
in fig. 1 state / resultant, the magnetization of the core part 2 is opposite in the direction of the resultant magnetization of the hollow part 3. This state is called the inverse state, in this inverse state the wall 4 of the domain forms the boundary between the core part 2 and the shell part 3. This boundary The unit is shown in FIG. 1 in the form of a cylindrical domain wall 4, although the domain boundary is a rather complex magnetic transition zone in the wire.
From a wire consisting of cobalt, iron and vanadium, pulses can be obtained, the magnitude of which is at least one order of magnitude greater than the magnitude of the pulses received from the wire from an alloy of nickel and iron. A preferred wire box for the wire of the invention is a composition containing about 45-55% cobalt, about 30-50% iron, and 4-14% vanadium.
For the manufacture of the proposed devices, a properly processed wire with a diameter is used. 0.25 mm. Wicker alloy wire has a composition containing about cobalt, about 10% vanadium, the rest, mainly iron, with some in secondary components, including manganese and silicon in amounts slightly lower than half a percent each.
The first scheme of the technological process of wire processing.
When using a 30 cm length of 0.25 mm wikalloy alloy wire, the preferred scheme of the work hardening process includes the following steps.
The first. The wire is stretched to its full length. A piece of wire 5 (Fig. 5) is secured on chuck 6 and It By means of a spring-loaded coil 8, the wire is stretched enough to straighten it, but without straightening it. Then, one cycle of deformation of the wire 5 by twisting is carried out, containing approximately 64 turns counterclockwise, and then approximately 48 turns clockwise. Tension is maintained during all stages of torsional deformation. The second. Further, 17.5 pts of wire deformation are performed in turns in each direction (8 turns counterclockwise, and then 8.5 turns clockwise make up one cycle). The cycle is repeated 17 times, after which
The second stage is completed with 8.5 turns counterclockwise. During this second stage, which normally lasts about 10-15 seconds, the 30 cm wire is continuously and 5 slowly pulled out: the magnitude of the elongation is in the range of 1-2%.
Third. The last stage of processing consists of another series of 8.5 turns each time, this time with an equal number of cycles and without additional stretching, but with maintaining the tension of the wire. During this stage, the number of cycles carried out in the second stage is repeated 3-4 times. It has been found that a good result is obtained when conducting about 60 cycles.
The wire is then cut into usable lengths of length 0, for example ,. 1-3 cm
The second process flow diagram.
For those applications where maximum time stability 5 is unimportant, a less preferred scheme is the technological process flow scheme. Processing the wire from wikalloy alloy, which includes the following steps (using a 30 cm piece of wire with a diameter of 0.25 mm).
First stage. The wire is stretched to its full length. The applied tensioning force holds the wire in-tempered until it is full. 5 lengths of condition without pulling it out. Next, one cycle of torsion wire deformation is performed, containing 14 turns counterclockwise, and then 12 turns 0 clockwise.
Second phase. Conducted 120 wire warp cycles of twelve Turns in each direction. SRI (12 turns counterclockwise 5 hands, and then 12 turns of
clockwise is one cycle). During this second stage of the technological process of deforming the wire, during the twisting of the wire it is stretched continuously. nph this 30 centimeter wire is slowly and continuously extended by about 3 mm.
The third stage. The last stage of processing consists of 12 cycles of 12 rounds each — 5 rotations counterclockwise and 12 turns clockwise without further stretching, but sustaining the tension of the wire,. whereby the elongation obtained in the second step is maintained.
Then the wire is cut into lengths of, for example, 1-3 cm.
In both schemes, the resultant tangential stress in one centric direction is significantly
exceeds the resultant tangential stress applied in a different cyclic direction. In particular, the first operation of each processing circuit provides this result.
The alloy used in both schemes of the process of strain hardening the wire is the same. Its stripping is annealed in order to obtain a homogeneous starting material, and I have sufficient viscosity for carrying out the process of strain hardening. The wire is preferably first annealed in order to obtain: a grainy / g structure, with 10,000 (or more) grains per 1 mm. This fine-grained structure ensures that the desired viscosity is obtained.
It was found that for both wire processing schemes, the fourth stage is also important. This fourth step is a heat treatment step. In the early stages of the experiments, the heat treatment was carried out at approximately 8 hours. However, it is sufficient to carry out the heat treatment stage for 4 hours approximately, which is advantageous due to the acceleration of the wire processing process. It is preferable to perform heat treatment, passing a current of 5.6 A through this wire with a diameter of 0.25 mm for 120 ms. Thermal processing gives a noticeable improvement in the exhaust signal, but more importantly, it reduces the risk of changing the characteristics of the wire during its use when exposed to a high-temperature environment. This fourth heat treatment stage after strain hardening ensures aging of the wire, which in turn ensures stability when used.
Wire testing technique and test results.
FIG. 2 schematically shows a test apparatus used to determine the output pulses that can be obtained using cobalt iron-vanadium wire according to the invention, and compared with the output pulses received from the nickel-nickel wire, to the transformer 9 is supplied from a line with a frequency of 60 Hz providing an alternating signal to the solenoid 10. Inside the solenoid 10 in its center there is a segment of wire 1 around which the sensing coil 11 is wound. 10 weave solenoid current creates in the center of the solenoid axial magnetic field.
The most pronounced output / impulses from a cobalt-iron nadium wire are obtained when the wire is reversal asymmetrically. The exciting field H acting on the wire 1 (FIG. 2) is shown in FIG. 3 curve 12, diode 13
10 passes the full positive half-cycle of the alternating signal with a frequency of 60 Hz, and the resistance of the branch 14 is adjusted so that it passes a much smaller negative
5 half-period, so that the exciting field acting on the wire 1 has a positive peak of 150 Oe, and the 6th significant peak is only about 20 E. The resistance of the branch 15 is em
0 is just current limiting resistance.
The hysteresis loop for wire 1 according to the invention excited in the manner described is shown by a curve
5 to 16 in FIG. 3 (the form that would have been visible to the oscilloscope) is shown. The breaks in curve 16 are visible on the oscilloscope only as a low luminosity, with a trace, because the rate of change of magnetic flux through the core part 2, when the intensity of the external H passes through the appropriate threshold value is very high.,
A larger discontinuity in curve 16 is observed when an external longitudinal magnetic field H reversals. the longitudinally magnetized core part from the reverse state (Fig. 1) to the coincident state,
0 A small discontinuity is observed when going from a state of coincidence to the opposite by reversing the external field of the core part of the coincidence. Impulse 17 (fig.z)
5 induced in the coil 11 by reversal. from the reverse state to the coincident state, much larger than the pulse 18 induced by the remagnetization from i
-0 matches in reverse.
For example, when using from; cutting the wire 1 with a length of 3 cm and perceived coil 11 with 925 turns of wire and outputting the output signal from the coil 11 in the load
A 1000 Ohm pulse 17 is more than IfS B and has a duration of about 20 ISS at half amplitude. And pulse 18 has comparable values of 125 mV and at least
60 ISS. Thus, under these conditions, the pulse amplitude 17 is 12 times the pulse amplitude 18, In an open circuit, a pulse is obtained
5 17 is more than 2V. When the excitation device creates a negative field H equal to 150 Oe and a positive field H equal to 160 Oe, two pulses 19 are obtained, equal to each other and opposite in polarity (see, Fig. 4). Each of these two pulses 19 has an amplitude of about 550 mV and a duration (width) of about 40 ISS with a half amplitude. Thus, with symmetric magnetic reversal, the two received pulses are equal to each other and have a significantly smaller value than the pulse 17, which is obtained at an optimum asymmetric reversal and core part. When using the circuit shown in FIG. 2, with the exception of elements 13 and 14, a sinusoidal exciting field (curve 20) will act on the wire, creating an external external field H, the strength of which varies from +150 to -150 E. The result is hysteresis loop 21 With a maximum positive field H, the shell part 3 and the core part 2 are magnetized in a positive direction, represented by the upper right corner of the hysteresis core 21. This can be considered a positive state of coincidence. When the external field H is reduced, the magnetization will decrease until, with a relatively small negative field H of about -12 o. Core part 2 does not change the I direction of its magnetization from positive to negative, Thus, the wire 1 is magnetized from coincidence to the opposite. In this case, a gap 21a is formed in the hysteresis loop 2. As a result, an output pulse of approximately 550 mV and a duration of 40 ISS appears on the sensing coil 11. With a further increase, the field H in the negative non-directing is achieved; the point at which the direction of the magnetization of the shell changes to the opposite, resulting in a small gap of 21 °. in the hysteresis loop 21 and the small output pulse 22, the Core and the sheath are now the B negative state, the H field reaches the negative peak, and then decreases in magnitude. When the field H becomes positive (about 12 Oe), the core part 2 changes the direction of the magnetization to positive, which is indicated by a break 21c t. This produces another output pulse 19, the amplitude of which is 550 mV and the duration 40 ISS. in the opposite state, the Field H continues its further enhancement in the positive direction until the moment when the b high part changes the direction of its magnetization / the result of which is small xoy output pulse 22 and return wire 1 in a positive state coincidence. Reversal from the reverse state to the coincidence state gives a large output pulse than the reversal from the coincidence state to the opposite one, to the first that occurs at a higher speed than the last. In the described embodiments, it is necessary for the core to change the direction of the exciting field H to the opposite. A simple complete removal of the exciting field H will not provide a reversal of the core part 2. This should be changed in the direction of the exciting field to the opposite to ensure the reversal of the core does not matter what the TYPE is; magnetization reversal: asymmetrical. (Fig, 3) or symmetric (Fig. 4). In contrast to sTOMj in the variants with iron-nickel wire, the latter automatically remagnetates from the same condition to the opposite when the excitation field is removed.
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权利要求:
Claims (2)
[1]
1. A magnetic device made in the form of a magnetic wire uniform in chemical composition, having a sheath and a core i part and having the ability to magnetize in an external magnetic field along its axis and be in a state of coincidence when the directions of magnetization of the sheath and core parts coincide, and the opposite state - when they are opposite, and the coercive force of the shell part is greater than the coercive force of the core part, which differs in that, in order to increase the sensitivity and to improve the signal-to-noise characteristic, the core part is designed so that it has a coercive force sufficient to ensure that a coincidence state is maintained in the absence of an external magnetic field, the relative magnetic properties of the core and shell parts being selected so that the device ^{1 is} switched from the reverse state in a state of coincidence through remagnetization of the core occurs faster than vice versa.
[2]
2. A method of manufacturing a magnetic device, including the operations of heat treatment *, cyclic deformation torsion of a magnetic wire under tension, and tfl, and wherein, in order to increase the sensitivity of the magnetic device, deformation torsion in one direction is performed to a greater extent than in another direction.

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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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US79339477A| true| 1977-05-03|1977-05-03|

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