• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
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    • 专利摘要:
    A method of measuring the range of environmental targets (Ui) by sweeping pulses reflected therefrom, in particular laser pulses, comprising: emitting pulses (2) having a pulse spacing (i) which is varied according to a modulation signal, as transmit pulses (Sm) and concomitantly recording the reflected ones Pulses as received pulses (En), determining a first sequence (F) of distance measurement values (Dk) of transit times (ATk) between transmit pulses (Sm) and such receive pulses (En), each within a first time window (Wm) after each transmit pulse (Sm ) and determining at least a second sequence (F1) of distance measurement values (Dk ') from transit times (ATk') between transmit pulses (Sm) and such receive pulses (En), each within a second time window (Wm ') after each transmit pulse (ATk'). Sm), and determining that sequence (F ') of range measurement values (Dk') which is least due to the modulation signal nflusst, as a result of the distance measurement.
    公开号:AT511310A1
    申请号:T494/2011
    申请日:2011-04-07
    公开日:2012-10-15
    发明作者:Peter Dipl Ing Rieger；Andreas Dr Ullrich
    申请人:Riegl Laser Measurement Sys；
    IPC主号:
    专利说明:

    PATENT OFFICER DIPL.-ING. DR.TECHN * ANDREAS WETSER EUROPEAN PATENT AND TRADEMARK A'ITORNEY A 1130 VIENNA - KOPFGASSF. 7 04044 RIEGL Laser Measurement Systems GmbH A-3580 Horn (AT)
    The present invention relates to a method for measuring the range of environmental targets by measuring the transit time of pulses reflected therefrom. The pulses can be of any kind, e.g. Light pulses, in particular laser pulses, radio pulses, in particular radar pulses, sound pulses or the like. The invention further relates to a method for laser scanning by directing laser pulses continuously to different environmental targets.
    Modern pulse duration rangefinders such as laser rangefinders or scanners operate with high pulse power over long distances and / or high pulse repetition rate for the rapid creation of a plurality of distance measuring points of the environment. In either case, the situation may arise that the next pulse is already being transmitted even before the reflection of the last pulse has been received, so that the incoming receive pulses can no longer be unambiguously assigned to their respective transmit pulse. This is known as "multiple time around" (MTA) or "multiple pulses in the air" problem. The maximum size d ^ ax of the clearly measurable distance range, the so-called MTA zone, results from the pulse repetition rate PRR and the speed of light c to dmax = c / (2 * PRR). THI (+ 45 1) 879 17 06 · FAX: (+43 1) 879 17 07 FMAll ,: ΜΛίΙ. @ ΓΛΤΙ .NTKNI'.T -WFB: WWW.PATI.NTF.NI.T l'.KSTI · ' , BANK: 038-56704 Β1.Ζ: 20111 · [BAN: ATI02011100003856704 · BKA GIBAATWW VAT: AT U 53832900
    For example, state-of-the-art laser scanners offer pulse repetition rates of up to 400 kHz, which corresponds to an MTA zone size d.nax of about 375 m. If this measuring distance is exceeded, the measurement result can not be correctly interpreted due to the ambiguous assignability of the transmit and receive pulses.
    Figs. 1 and 2 show this situation in detail. From an aircraft-based laser scanner 1, a pulsed laser measuring beam 2 is scanned across an environment U with individual environmental targets (sampling points) Ui., U2, ..., e.g. fan-shaped line by line. From transit time measurements at the individual emitted pulses Si, S2,..., Which are retrieved after the ambient reflection as received pulses Ei, E ,..., The target distances Di, D ,... To the individual environmental targets Ui, U -, ... are determined.
    1a and 2a show an exemplary situation in the measurement of environmental targets Ui, U2, which lie in the first, the laser scanner 1 nearest MTA zone Z: The transmission pulse belonging to the receive pulse Εχ is recovered before the next transmit pulse S2 in the time interval τ = 1 / PRR is sent, etc., etc.
    FIGS. 1b and 2b show an exemplary situation when environmental targets Ux ', U4 * lie in the second MTA zone Z': Here, the receive pulse E3 belonging to the transmit pulse S3 is received only after the second transmit pulse S2 has already been transmitted. To determine the correct distance D3 'of the 3 3
    4 «· 4« ·· • «· • 4 * * • · • · · * ·« · ·
    Surrounding target U3 'in the zone Z', it is necessary to correctly assign the received pulse E3 to the transmit pulse S3; if the receive pulse E3 is erroneously assigned to the immediately preceding transmit pulse S4, an incorrect target range D3 results in the wrong MTA zone Z instead of the correct target range D3 'in the correct MTA zone Z'.
    For correct mutual assignment of the transmit and receive pulses and thus overcome the MTA zone limits for clear distance measurement results a variety of methods are known. A first option is to make sure that all expected environmental targets are in one and the same MTA zone when planning the survey task, so that the correct assignment can be made. This method is naturally only applicable for special measuring tasks and e.g. for highly mobile or large-scale surveying or scanning tasks, e.g. the airborne scanning of mountains or terrestrial vehicle-based scanning, unsuitable.
    Another group of methods is based on making the individual transmission pulses distinguishable by varying their polarization, amplitude or wavelength in order to be able to assign the received pulses accordingly. However, these methods are either only for a few "pulses in the air". suitable or require complex coded pulses, which limits each of the pulse repetition rate and the measurable distance range and extends the measurement time. 4
    ··· «·« # »* · • · ·« *
    The invention has for its object to provide a method for distance measurement or scanning, which allows automatic assignment and thus correct measurement of environmental targets in any MTA zones. This object is achieved by a method of the initially mentioned kind, which comprises:
    Transmitting pulses having a pulse interval which is varied in accordance with a modulation signal as transmission pulses and accompanying recording of the reflected pulses as reception pulses,
    Determining a first sequence of ranging values from transit times between transmit pulses and such receive pulses, each received within a first time window after each transmit pulse, and
    Determining at least a second sequence of ranging distances from transit times between transmit pulses and such receive pulses, each received within a second time window after each transmit pulse, and
    Determining that sequence of distance measurement values, which is least affected by the modulation signal, as a result of the distance measurement.
    It should be noted that the variation of the pulse interval and thus the pulse repetition rate (reciprocal value of the pulse interval) as so-called "PRR modulation". is known per se in the field of radar technology to identify "ghosting" of transmit pulses outside the proper MTA zone.
    The present invention is based on the surprising finding that by a signal analysis evaluation of at least two possible sequences ("candidate sequences") of distance measurement values, as obtained for different time window recording variants of received pulses, the "correct". Distance measurement sequence can be determined automatically, u.zw. by detecting the influences of the pulse spacing or PRR modulation signal in the candidate sequences. As a departure from previously known methods, a wide variety of possible distance measurement value sequences corresponding to MTA zone assignments are evaluated on the modulation signal fed in at the beginning.
    The length of the first and second time windows is preferably approximately equal to the average pulse spacing of the transmitted pulses. As a result, the time windows each cover exactly one MTA zone. It is furthermore particularly advantageous if the first and second time windows are each offset by an integral multiple of the average pulse spacing of the transmitted pulses, so that the measurable MTA zones can be connected to one another to a large extent without any gaps.
    The method of the invention can be extended to any number of MTA zones by performing more than two pairings of transmit and receive bursts
    Using more than two different time windows are formed and accordingly more than two candidate sequences of distance measurement value sequences are generated, from which the modulation signal is least affected. The greater the period of the modulation signal and the more different time windows are possible, the greater the number of MTA zones, which can be detected and assigned in this way. In this sense, according to a first preferred embodiment, the injected modulation signal is a random signal (noise), i. from "infinite" Period.
    Since in practice an automatic evaluation of a limited number of MTA zones is sufficient, the modulation signal can also be only a pseudo-random signal with a limited period (pattern or code length). Particularly suitable for this purpose is a signal based on a Barker code, which brings advantageous properties for the selection of the candidate distance measurement value sequences.
    Determining the least-value sequence of values influenced by the PRR or pulse interval modulation can be carried out in various ways. In accordance with a first preferred embodiment, signal energies of the various candidate range value sequences are calculated for this purpose and the sequence with the lowest signal energy is selected. This embodiment takes advantage of the fact that pulse spacing modulation always results in an increase in the signal energy of those rangefinder value sequences in which it is reflected.
    A preferred variant of this embodiment is to compute autocorrelations of the range measurements and to select that sequence as the correct one which shows the highest autocorrelation. This variant is based on the knowledge that the least-influenced candidate sequence has the greatest self-similarity (autocorrelation).
    Another preferred alternative is to calculate cross-correlations between the candidate ranging results and the modulation signal and to select the sequence with the least cross-correlation as the correct distance measurement result.
    Yet another preferred variant is that the distance measurement value sequences are frequency-analyzed and the sequence with the lowest high-frequency content is selected as the correct one. This variant is based on the assumption that a modulation-related "roughness" in the "wrong" rangefinder sequences is usually higher-frequency than corresponds to the actual roughness of the measured environment.
    According to a first aspect of the invention, the method may be used for MTA-correct distance measurement of an environmental target by continuously directing the transmit pulses to that same environmental target. -. Q_ * «« * «··· · * * ^ ··· *« ·· «* * * a« t »« »*
    According to a second aspect of the invention, the method may also be used for laser scanning in that the transmit pulses are laser pulses and are continuously directed at different environmental targets to point scan an entire environment. Laser pulses can be directed by rotating mirror od. Like. Particularly simple to different goals.
    The invention will be explained in more detail with reference to embodiments illustrated in the accompanying drawings. In the drawings shows:
    Fig. 1 shows schematically various reflection situations of a pulsed laser scanning beam on environmental targets located in different MTE zones, according to the prior art;
    FIG. 2 shows exemplary time diagrams of transmit and receive pulses for the reflection situations of FIG. 1 according to the prior art; FIG.
    3 shows exemplary timing diagrams of transmit and receive pulses in connection with various steps of the method of the invention;
    FIG. 1 shows in detail exemplary candidate sequences of distance measurement values that occur during the method of the invention; FIG.
    Fig. 5 shows different variants of assignment steps between transmit and receive pulses in the context of the method of
    Invention; 9 • *
    Fig. 6 is a synopsis of the range measurements of Fig. 5 over a larger number of measurements;
    7 shows a first variant of the evaluation of the distance measurement sequences of FIG. 6 by calculating signal energies, here by means of a sliding standard deviation;
    8 shows a second variant of the evaluation of the distance measurement value sequences of FIG. 6 by calculating signal energies, here by means of autocorrelation;
    9 shows a third variant of the evaluation of the distance measurement value sequences of FIG. 6 by means of analysis of their autocorrelation properties; and
    10 shows the variant of FIG. 9 when using a bar-ker code as a modulation signal instead of a noise signal.
    FIGS. 1 and 2 show the impulse allocation problem of MTA-zone-exceeding rangefinding or scanning areas and have already been discussed at the beginning. To overcome this problem, the method now described below, which is based on a signal analysis of a plurality of transmission pulses Si, S2, S3, ..., in general Sm, and receive pulses E], Ej, E3, ..., generally En, is used ,
    The following process description concretely refers to laser pulses as transmit and receive pulses Sm, En reference. However, it will be appreciated that the transmit and receive pulses Sm, En can be of any type, for example sonic pulses in a sonar device, light pulses in a time-of-flight camera, photonic mixing device (PMD), Radar pulses in a radar range finder or scanner, electrical impulses in line gauges, etc., or just laser pulses in a laser range finder or scanner. Accordingly, the method described herein is generally applicable to any type of pulse transit time measurement method.
    Referring to Fig. 3a, a plurality of laser transmit pulses Sm from the laser rangefinder or scanner 1 are emitted to the environment U (Fig. 1) to recover a plurality of receive pulses En through reflections of the transmit pulses Sra at ambient targets U-. From the transit time ΔΊ1 of each ambient-reflected laser pulse, i. the difference between the reception time Tn of the received pulse Eri and the transmission time Tm of the underlying transmission pulse Sm, the distance D * = οΔΤ ·.: / 2 from the distance meter or scanner 1 to the measured environmental target Ui can be calculated in a known manner. The transit times ATk and distance readings Dk are directly proportional to each other and are therefore used synonymously and interchangeably in the following.
    Assuming a certain assignment ("pairing") P of a reception pulse Ec to a transmission pulse Sn, which will be discussed in more detail later on, it is possible to set a delay ΔΤ] for each pair of transmission pulse Sm and reception pulse Eu. and calculate a distance measurement value Dk. For a sequence S of transmission pulses (Sn, Sm + i, S-v + 2,... Sm +; i} and a sequence E of reception pulses {En, En + i, En + , ... Em, N} Thus a sequence F 11 * Λ of distance measurements {Dv, D2, D3, ... Dk, ... DN} can be calculated.
    The method described here can be used both for distance measuring, if the transmission pulses Sra are continuously directed to one and the same environmental target Ui, as well as for scanning, if the transmission pulses Sm are continuously directed to different environmental targets Uj, e.g. line by line scanning the environment U out. In the former case, a plurality of range measurements Dk of the same environmental target Ui are obtained, which are subsequently - e.g. adjusted to outlier values - can be averaged to obtain a final result of distance D. In the second case, a discrete surface model of the environment U (a "point cloud") can be created from the multiplicity of distance measurement values Dk and the emission direction Sm known in the scanner 1, as is known to the person skilled in the art, e.g. common in the field of laser scanning.
    Fig. 3b shows another form of assignment or pairing P 'between transmit pulses Sm and receive pulses E: i. The assignment P 'is based on the assumption that the environmental targets Ui are located in the second MTA zone Z' (FIG. 1), see the exemplary environment targets U3 'and U4'. In the assignment P ', a receive pulse E "is no longer assigned to the immediately preceding transmit pulse Sm but to the penultimate transmit pulse Sn_i to obtain a sequence of runtimes 12 from the difference of the receive and transmit times Tn-Tm_i, Tn + 1-Tn, etc. * · Λ ·
    • t I • ·
    • φ ι II «*« · * «« · ··· · a · ♦ · ΔΤι ', ΔΤ2', Δίν, ... and thus a new sequence F1 of distance measurement values {Di1, D2 ', D3', .. To get Dk ', ...}. If the measured environmental targets Ui are in the "correct" corresponding to the assignment P '. MTA zone Z ', the sequence F' with the distance measurement values Dk 'reproduces their distances correctly.
    In general, the MTA zone Z, Z ', Z " etc., in which the environmental targets Ui are not known. In this case too, in order to recognize the correct MTA zone position and thereby obtain the correct distance measurement values Dk, Dk ', Dk " etc., the following procedure is used.
    As shown in Figs. 3a and 3b, the transmission pulses Sm are not transmitted at a constant pulse spacing τ = 1 / PRR, i. a constant pulse repetition rate PRR, but with a pulse interval varying from transmit pulse to transmit pulse τχ = 1 / PRRx, τ2 = 1 / PRR2 etc., generally τι = 1 / PRRi. In other words, the pulse repetition rate PRR or the pulse interval 1 is modulated with a signal {"pulse position modulated") in order to achieve the mentioned variation of the pulse intervals ii.
    The variation of the pulse spacing τχ from pulse to pulse is preferably only slightly, for example +/- 1%, +/- 5% or +/- 10% around the mean (average) pulse spacing τ.
    The modulation signal for achieving said pulse spacing variation may be of any type, e.g. a sine wave, triangular, sawtooth, staircase, on
    Data signal with its own information content, etc. Preferably, the modulation signal is a random statistical signal such as white noise. With such a random signal, the pulse repetition rate PRRi or the pulse spacing n is in the manner of a random "phase jitter". the transmission pulses Sn randomly varies randomly. Within certain limits, such a random signal may also be merely pseudo-random, such as the Barker code discussed later.
    Due to the periodic or preferably random jitter caused by the modulation of the timings Tm of the transmission pulses S ^, different sequences F, F ', F ", ..., etc. of range measurements Dk, Dk', Dk " for different assignments P, P ', P ", ..., depending on the MTA zone location Z, Z', Z", ... of the environmental targets Uk different properties. This is shown in Figure 4 for four different assignments P, P ', P ", P, M resulting in four different range value sequences F, F', F ", F " range finders Dk, Dk ', Dk ", Dk " which are each plotted over their impact index (time index) k. The modulation signal in the present case was a random signal (noise signal), and the environmental targets Ui were in the present case in the second MTA zone Z '.
    As can be seen from Fig. 4, the PRR pulse pitch modulation noise is reflected in all sequences F, F ', F ", F ". with the exception of the "right" Distance measurement sequence F1 down, i. the distance measurement sequence F 'representing the correct MTA zone Z' is least affected by the modulation signal. This is due to the fact that the "right" Assignment P 'measures the transit times LTV between the receive pulses Er. + I, Er. + 2,... And their causative transmit pulses Sm, regardless of the jittered phase position Tm of the respective transmit pulse, whereas the modulation-induced phase position variations for "false". Assignments P, P ", Pzu respectively modulated and (here :) noisy " false " Durations ATk, LT: t ", ATV " etc. lead. Thus, by signal analysis evaluation of the received measurement value sequences F, F ', F ", F " the correct MTA zone, here Z ', detected and thus the correct distance measurement result, here F1, automatically determined.
    According to FIG. 5, in principle a wide variety of mappings P, P ', P ",... Can be formed in order to obtain a wide variety of potential removal measurement results F, F', F",... As candidate sequences for the subsequent evaluation and determination to generate the correct range order. It is irrelevant whether a first sequence S of transmit pulses Sm is in each case paired with a wide variety of second sequences E, E ', E ", ... of receive pulses En, see FIG. 5, or a first sequence E of receive pulses En with various second sequences S, S ', S ", ... of transmission pulses S 1, see FIG. 5 b, or generally different sequences S, Ξ', S",... of transmission pulses Sm with different sequences E, E ' , E ", ... of received pulses £ n, see Fig. 5c. The time interval ("offset") between the transmission and reception pulse sequences of an assignment P, P ', P ",... Determines, as explained below, in each case the MTA zone Z, Z ', Z ", ..., for which the assignment applies.
    Returning to Fig. 3, the assignments P, P ', P ", ... between the transmission pulses Sm and the reception pulses En can be established in the following manner. For the first assignment P, those received pulses En are taken into account and respectively assigned to their preceding transmit pulse Sm, which were received in each case within a first time window after the relevant transmit pulse Sm. By way of example, FIG. 3a shows three first time windows Wm, Wm + 1, Wm + 2 whose length is approximately equal to the average pulse spacing τ of the transmission pulses Sm and which respectively start directly at the time of transmission Tn of the relevant transmission pulse Sn (or possibly by a small pulse interval Value Δ later, see below). Thus, the delays ÄTk and thus distance measurement values Dk of the first sequence F are respectively formed between a transmission pulse Sm and the next reception pulse Er. This results in the assignment P for the measurement of the first MTA zone Z.
    By way of example, Fig. 3b shows two time windows Wm ', Wm + v' of second time windows Wra ', Wm + 1', Wmi; 1 / · which are opposite to the first time windows Wn < Wn + i ', Wm + 2', ... are offset by approximately an average pulse spacing τ of the transmission pulses Sm. The second time windows Wn ', Wm, i', Wm + 21, ... again have approximately the length of an average pulse interval τ and each begin at a predetermined distance (Offset) Off 'to the 16 * · 16 * · • * ♦ * »· •» · · · • λ · · * * · • ♦ · · · · i * * · ·
    Transmission times Tm, Tn, + 1, Tra + 2, ... the transmission pulses Sm, S ^ i,
    Sm you are referring to. The reception pulses En, i, Εη * 2, En + 3,... That arrive in the second time windows W * ', Wn + i' / Wm + 2 ',... Form the second sequence E', and the transit times ATk ' with respect to said penultimate transmit pulses Sm, Sm + :, Sm + 2 / - and thus distance readings Dk 'form the second sequence F' for measuring the second MTA zone Z '.
    The predetermined distance Off, Off, Off ", ... between the transmit pulses Sm and the start times of the respective time windows W; tl, Wm ', wn",... For the receive pulses En to be allocated to the transmit pulses Sm is preferably an integer multiple the average pulse interval τ, possibly increased by a small value .DELTA., in order to ensure that the time windows between the transmission pulses Sm come to lie in order to exclude disturbances of transmission pulses Sn to a receiving electronics for the received pulses. Thus, the predetermined distance Off for the assignment P is preferably equal to O-τ + Δ, the distance Off 'for the assignment P' is equal to l-τ + Δ, the distance Off " for the assignment P " equal to 2 · τ + Δ, etc., etc.
    By taking into account only those received pulses En that fall within the respective time windows Wm, Wm ', gaps in the receive sequences E, E', E ", ... which can be reduced to" lost ", e.g. of non-reflective targets "swallowed" " In this case, there is no reception pulse Sm for a reception * ft * ft "ft * ft * ft 17 * ft * ft" ft ft "ft 4 I 14 "ft ft ft ft 4 ft ft ft" 4 * * 4 ft "4 ft # ·« * "5 ··" "" # * pulse Et in the considered time window Wm, so that there is no determinable running time ΔΤν , ATt ', ... and no distance measurement DDk', .... Such missing individual distance measurement values in the sequences F, F ', FM, ... are not statistically significant in their statistical evaluation, ie lead to no significant impairment of the evaluation result.
    Fig. 6 shows the ranging results F, F ', F ", F " of Fig. 5 again over a larger number of indices k or a longer period in synopsis or parallel representation. Again, it can be seen that the second ranging sequence F 'is the least noisy, i. E. the least influence by the modulation signal (here: noise) shows.
    On the candidate range value sequences F, F ', F ", F1 " For example, any signal analysis method known in the art can be used to obtain the least-affected modulation signal, e.g. least noise, range measurement sequence F 'as the correct range finding result of the environmental targets Uj. to investigate. FIGS. 7 to 10 show a few variants of suitable evaluation methods.
    Fig. 7 shows an analysis of the range value sequences of Fig. 6 by calculating a sliding standard deviation σ over a sliding time window of e.g. 100 readings. The standard deviation σ shows an average-adjusted energy measure of the sequences F, F ', F ", Fm, where the sequence F' with the lowest signal energy is selected as the measurement result. It 18th
    it is understood that other energy measures than a standard deviation used can be calculated; the energy analysis is based on the postulate that any modulating signal initially input to the transceiver pulses Sn will always result in a detectable energy increase of the distance measurement value sequences F, F ", F " leads.
    Fig. 8 shows the calculation of autocorrelation functions AKF of the range value sequences F, F'f F ", F " of the example of FIG. 6 over the autocorrelation offset index δ. The autocorrelation at 6 = 0 is again a measure of the signal energy of the range finding sequence, and the range measure F 'with the lowest autocorrelation AKF (5 = 0) is the correct measure.
    FIG. 9 shows autocorrelation functions AKFo of the distance measurement value sequences F, F1, F ", F1" normalized to the signal energy. of the example of Fig. 6. For a given auto-correlation offset index δ not equal to zero, e.g. δ = 5, the autocorrelation of the individual sequences is different; The correct range finding sequence F *, being least affected by the PRR modulation, is "most similar to itself". and thus has the highest autocorrelation AKFo at δ 4- 0 compared to all others, "false". Distance measurement sequences F, F ", F, n.
    FIG. 10 shows the same autocorrelation evaluation as FIG. 9 when using a pseudo-random signal instead of a noise signal, here a Barker code of code length eleven (+1 19 -1 +1 +1 -1 -1 +1 -1 -1 +1 - 1) as a modulation signal. Between the code repeat points, i. the multiple of the code length eleven, the signal spacing (the separation) between the autocorrelation values of the individual sequences is increased. With an autocorrelation offset 5 = 5 lying approximately in the middle of the code length, the correct sequence F 'can thus be more easily distinguished from the other sequences F, F ", F'". be separated and detected as in the variant of Fig. 9.
    Another variant of the evaluation of the range value sequences F, F ', F ", F"' is to cross-correlate each sequence with the modulation signal. The least cross-correlation sequence is the one in which the modulation is the least effective, and thus the correct distance measurement result.
    Yet another variation is to use the ranging results F, F ', F ", F " Frequency analysis, for example by means of FFT (Fast Fourier Transformation) to detect known frequencies of the modulation signal therein or simply to determine the amount of high-frequency components in the sequences. The latter is based on the assumption that noise modulations, Barker code modulations, etc., contribute to amplified high frequency components in the " false " Guide distance measurements. The sequence with the lowest high-frequency components is then selected as the correct distance measurement result. 20:
    The invention is not limited to the illustrated embodiment forms, but includes all variants and Modifi cations that falls within the scope of the attached claims len.
    权利要求:
    Claims (12)
    [1]
    1. A method for the distance measurement of environmental targets by transit time measurement of pulses reflected therefrom, in particular laser pulses, comprising: emitting pulses ¢ 2) with a pulse spacing (τ) which is varied according to a modulation signal, as transmit pulses (Sm) and accompanying recording of the reflected pulses as receive pulses {En), determining a first sequence (F) of ranging measurements (D; J of propagation times {ΔΤ *) between transmit pulses (Sm) and such receive pulses (En), each within a first time window (Wm) after each Transmitting pulse (Sm) are received, and determining at least a second sequence (Fr) of distance measurement values (D}: 1} of transit times (ΔΤ * ') between transmit pulses (Sr) and such received pulses (En), each within a second time window ( W ^ ') are received after each transmission pulse (Sm), and determining that sequence {F') of range measurement values (D * ') which are given by the Modulation signal is least affected as a result of the distance measurement.
    [2]
    2. The method according to claim 1, characterized in that the length of the first and second time windows (Wra, Wn ·. ') Each approximately equal to the average pulse interval (x) of the transmission pulses (S ^). 22 • 4 *
    [3]
    3. The method according to claim 1 or 2, characterized in that the first and second time windows (W ,,., Wm ') to each other by about an integer multiple of the average pulse spacing (τ) of the transmission pulses (Sm) are offset.
    [4]
    4. The method according to any one of claims 1 to 3, characterized in that the modulation signal is a random signal.
    [5]
    5. The method according to any one of claims 1 to 3, characterized in that the modulation signal is a pseudo-random signal.
    [6]
    6. The method according to claim 5, characterized in that the modulation signal is based on a Barker code.
    [7]
    A method according to any one of claims 1 to 6, characterized in that determining the least affected sequence (F1) by calculating signal energies (σ) of the sequences (F, F ', F ", F'") and selecting the sequence with the lowest signal energy.
    [8]
    8. Method according to one of claims 1 to 6, characterized in that the determination of the least affected sequence (F ') by calculating autocorrelations (AKF) of the sequences (F, F', F ", F '") and selections the sequence with the highest autocorrelation occurs.
    [9]
    9. The method according to any one of claims 1 to 6, characterized in that the determination of the least affected sequence (F ') by calculating cross-correlations of the sequences

    (F, F ', F ", F'") is performed with the said modulation signal and selections of the sequence with the lowest cross-correlation.
    [10]
    A method according to any one of claims 1 to 6, characterized in that determining the least affected sequence {F ') by frequency analyzing the sequences (F, F', F ", F '") and selecting the sequence with the lowest high frequency Shares.
    [11]
    11. The method according to any one of claims 1 to 10, wherein the transmission pulses (Sm) are continuously directed to the same environmental target (U,).
    [12]
    12. The method according to any one of claims 1 to 10 for laser scanning, wherein the transmission pulses (Sn) are laser pulses and are continuously directed to different environmental targets (U.).
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    同族专利:
    公开号 | 公开日
    EP2694996A1|2014-02-12|
    WO2012135874A1|2012-10-11|
    CA2828441C|2018-01-02|
    AU2011364939B2|2016-04-14|
    AT511310B1|2013-05-15|
    CA2828441A1|2012-10-11|
    AU2011364939A1|2013-10-03|
    US20120257186A1|2012-10-11|
    US9268013B2|2016-02-23|
    EP2694996B1|2015-03-25|
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    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    ATA494/2011A|AT511310B1|2011-04-07|2011-04-07|PROCESS FOR REMOTE MEASUREMENT|ATA494/2011A| AT511310B1|2011-04-07|2011-04-07|PROCESS FOR REMOTE MEASUREMENT|
    EP11767596.7A| EP2694996B1|2011-04-07|2011-09-15|Method for measuring distance|
    PCT/AT2011/000377| WO2012135874A1|2011-04-07|2011-09-15|Method for measuring distance|
    CA2828441A| CA2828441C|2011-04-07|2011-09-15|Method for measuring distance|
    AU2011364939A| AU2011364939B2|2011-04-07|2011-09-15|Method for measuring distance|
    US13/242,446| US9268013B2|2011-04-07|2011-09-23|Method for measuring distances|
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