CN110426700B - Ranging method for 24GHz millimeter waves - Google Patents

Ranging method for 24GHz millimeter waves Download PDF

Info

Publication number
CN110426700B
CN110426700B CN201910673702.9A CN201910673702A CN110426700B CN 110426700 B CN110426700 B CN 110426700B CN 201910673702 A CN201910673702 A CN 201910673702A CN 110426700 B CN110426700 B CN 110426700B
Authority
CN
China
Prior art keywords
path
frequency signal
radio frequency
signal
intermediate frequency
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN201910673702.9A
Other languages
Chinese (zh)
Other versions
CN110426700A (en
Inventor
朱新平
卢煜旻
朱欣恩
李成进
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Sijie Microelectronics Xiamen Co ltd
Original Assignee
Shanghai Silicon Microelectronics Co ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shanghai Silicon Microelectronics Co ltd filed Critical Shanghai Silicon Microelectronics Co ltd
Priority to CN201910673702.9A priority Critical patent/CN110426700B/en
Publication of CN110426700A publication Critical patent/CN110426700A/en
Application granted granted Critical
Publication of CN110426700B publication Critical patent/CN110426700B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/02Systems using reflection of radio waves, e.g. primary radar systems; Analogous systems
    • G01S13/06Systems determining position data of a target
    • G01S13/08Systems for measuring distance only
    • G01S13/32Systems for measuring distance only using transmission of continuous waves, whether amplitude-, frequency-, or phase-modulated, or unmodulated
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02DCLIMATE CHANGE MITIGATION TECHNOLOGIES IN INFORMATION AND COMMUNICATION TECHNOLOGIES [ICT], I.E. INFORMATION AND COMMUNICATION TECHNOLOGIES AIMING AT THE REDUCTION OF THEIR OWN ENERGY USE
    • Y02D30/00Reducing energy consumption in communication networks
    • Y02D30/70Reducing energy consumption in communication networks in wireless communication networks

Abstract

The invention relates to the technical field of communication, in particular to a ranging method of 24GHz millimeter waves, which comprises the following steps: step S1, transmitting a first radio frequency signal through an antenna group; s2, receiving a second radio frequency signal formed by reflecting the first radio frequency signal through the antenna group; s3, forming two paths of intermediate frequency signals by the first radio frequency signal and the second radio frequency signal through a frequency mixing method; s4, acquiring two paths of voltage signals through two paths of intermediate frequency signals; and S5, analyzing the two paths of voltage signals to acquire the distance information between the antenna group and a measured object. The technical scheme of the invention has the beneficial effects that: the distance measuring method for 24GHz millimeter waves can measure the target distance of a shorter distance (less than 60 cm), can achieve the distance measuring precision of + -1mm, does not need a complex processing process, correspondingly reduces the requirements of software and hardware, reduces the cost and is suitable for popularization.

Description

Ranging method for 24GHz millimeter waves
Technical Field
The invention relates to the technical field of communication, in particular to a ranging method for 24GHz millimeter waves.
Background
24GHz millimeter wave ranging is widely applied to the fields of traffic, hydrology and the like which need ranging. The conventional 24GHz millimeter wave generally adopts a frequency modulation continuous wave mode to measure the distance, and the distance to be tested is calculated through the spectrum phase analysis of two paths of intermediate frequency signals.
However, due to the presence of the frequency modulation signal, the test method is difficult to measure the frequency spectrum of the intermediate frequency signal smaller than the frequency of the modulation signal, the 24GHz band bandwidth of the ISM (Industrial Scientific Medical industrial scientific medical) is limited, and only the range of 250MHz can be used, so that objects within 60cm cannot be tested. Because of the frequency modulation continuous wave ranging mode, the measurement accuracy is limited by bandwidth, and although the accuracy can be improved through curve fitting, larger calculation capability is required. The hardware requires a complex modulation circuit, the software requires a strong DSP (Digital Signal Processing digital signal processing) processing capability, for example, complex fourier transform processing is required, and the cost is high. Therefore, the above problems are a major problem for those skilled in the art.
Disclosure of Invention
In order to solve the problems in the prior art, a 24GHz millimeter wave ranging method is provided. The specific technical scheme is as follows:
the invention provides a ranging method of 24GHz millimeter waves, which comprises the following steps:
step S1, transmitting a first radio frequency signal through an antenna group;
s2, receiving a second radio frequency signal formed by reflecting the first radio frequency signal through the antenna group;
s3, forming two paths of intermediate frequency signals by the first radio frequency signal and the second radio frequency signal through a frequency mixing method;
s4, collecting two paths of voltage signals through the two paths of intermediate frequency signals;
and S5, analyzing the two paths of voltage signals to acquire the distance information between the antenna group and a measured object.
Preferably, in the step S3, the two intermediate frequency signals are subjected to filtering processing.
Preferably, the mixing method is a zero intermediate frequency quadrature mixing method.
Preferably, in the step S3, the two intermediate frequency signals are an I intermediate frequency signal and a Q intermediate frequency signal, respectively.
Preferably, the first radio frequency signal is denoted as ftx=asin (ax), the second radio frequency signal is denoted as frx=bsin (ax+y), and the I-path intermediate frequency signal and the Q-path intermediate frequency signal are generated by mixing the first radio frequency signal and the second radio frequency signal, wherein a specific formula of the I-path intermediate frequency signal is as follows:
Asin(ax)*Bsin(ax+y)*L;
the specific formula of the Q paths of intermediate frequency signals is as follows:
Asin(ax)*Bcos(ax+y)*L;
wherein A is used for representing the amplitude of the first radio frequency signal;
b is used to represent the amplitude of the second radio frequency signal;
ax is used to represent frequency;
y is used to represent the amount of phase shift;
l is used to represent the mixing attenuation coefficient.
Preferably, in the step S4, the I-path intermediate frequency signal and the Q-path intermediate frequency signal are used to collect an I-path direct current voltage signal and a Q-path direct current voltage signal, respectively.
Preferably, in the step S5, the frequencies and phases of the I-path dc voltage signal and the Q-path dc voltage signal are analyzed to calculate the distance information between the antenna group and the measured object.
Preferably, the first radio frequency signal generates the 24GHz millimeter wave signal.
The technical scheme of the invention has the beneficial effects that: the distance measuring method for 24GHz millimeter waves can measure the target distance of a shorter distance (less than 60 cm), can achieve the distance measuring precision of + -1mm, does not need a complex processing process, correspondingly reduces the requirements of software and hardware, reduces the cost and is suitable for popularization.
Drawings
Embodiments of the present invention will now be described more fully with reference to the accompanying drawings. The drawings, however, are for illustration and description only and are not intended as a definition of the limits of the invention.
FIG. 1 is a flow chart of steps of an embodiment of the present invention;
fig. 2 is a waveform diagram of an embodiment of the present invention.
Detailed Description
The following description of the embodiments of the present invention will be made clearly and completely with reference to the accompanying drawings, in which it is apparent that the embodiments described are only some embodiments of the present invention, but not all embodiments. All other embodiments, which can be made by those skilled in the art based on the embodiments of the invention without making any inventive effort, are intended to be within the scope of the invention.
It should be noted that, without conflict, the embodiments of the present invention and features of the embodiments may be combined with each other.
The invention is further described below with reference to the drawings and specific examples, which are not intended to be limiting.
The invention provides a ranging method of 24GHz millimeter waves, which works an antenna group in a continuous wave mode without modulation, wherein the ranging method comprises the following steps:
step S1, transmitting a first radio frequency signal through an antenna group;
s2, receiving a second radio frequency signal formed by reflecting the first radio frequency signal through the antenna group;
s3, forming two paths of intermediate frequency signals by the first radio frequency signal and the second radio frequency signal through a frequency mixing method;
s4, acquiring two paths of voltage signals through two paths of intermediate frequency signals;
and S5, analyzing the two paths of voltage signals to acquire the distance information between the antenna group and a measured object.
The first radio frequency signal is denoted as ftx=asin (ax), the second radio frequency signal is denoted as frx=bsin (ax+y), and the first radio frequency signal and the second radio frequency signal are mixed to generate an I-path intermediate frequency signal and a Q-path intermediate frequency signal, wherein the specific formula of the I-path intermediate frequency signal is as follows:
Asin(ax)*Bsin(ax+y)*L;
the specific formula of the Q paths of intermediate frequency signals is as follows:
Asin(ax)*Bcos(ax+y)*L;
wherein A is used for representing the amplitude of the first radio frequency signal;
b is used to represent the amplitude of the second radio frequency signal;
ax is used to represent frequency;
y is used to represent the amount of phase shift;
l is used to represent the mixing attenuation coefficient.
According to the ranging method for 24GHz millimeter waves, as shown in fig. 1, the antenna group is used for transmitting the first radio frequency signal, and the first radio frequency signal is reflected by the measured object to form the second radio frequency signal, and then the second radio frequency signal is received by the antenna group.
Further, the first radio frequency signal and the second radio frequency signal are subjected to zero-crossing intermediate frequency quadrature mixing operation to form two paths of intermediate frequency signals which are intersected, and then the two paths of intermediate frequency signals are subjected to filtering processing, and then two paths of voltage signals are acquired.
The two intermediate frequency signals are respectively an I intermediate frequency signal and a Q intermediate frequency signal, and the I intermediate frequency signal and the Q intermediate frequency signal are respectively used for collecting an I direct current voltage signal and a Q direct current voltage signal through an ADC (Analog-to-digital converter Analog-to-digital converter), wherein the I direct current voltage signal and the Q direct current voltage signal are changed along with the change of the phase.
The ADC adopts a 16-bit ADC to respectively collect I paths of direct current voltage signals and Q paths of direct current voltage signals so as to reduce cost.
In addition, it should be noted that, when the measurement is started, the antenna set needs to perform environmental calibration, and the distance between the measured object is fixed first to obtain reference voltage signals VrefI and VrefQ of the I-path direct current voltage signal and the Q-path direct current voltage signal when the measured object is not present, where VrefI is the I-path reference voltage signal and VrefQ is the Q-path reference voltage signal, so as to be used as a subsequent calculation calibration basis.
Further, the frequencies and phases of the I path direct current voltage signal and the Q path direct current voltage signal are respectively analyzed to calculate the distance between the antenna group and the measured object, so that the distance measuring precision is higher and the cost is lower.
In this embodiment, in step S5, the frequencies and phases of the I-path dc voltage signal and the Q-path dc voltage signal are analyzed to calculate the distance information between the antenna group and the measured object.
The specific way of calculating the distance between the antenna group and the measured object is as follows:
if the moving distance of the measured object is D, D is the measured distance, the I path voltage signal acquired after the measured object moves is VI, and the Q path voltage signal is VQ.
Assuming that the first rf signal is ftx=asin (ax), and the second rf signal reflected by the measured object is frx=bsin (ax+y).
Further, the first radio frequency signal and the second radio frequency signal are mixed to generate an I-path intermediate frequency signal and a Q-path intermediate frequency signal, wherein the specific formula of the I-path intermediate frequency signal is as follows:
Asin(ax)*Bsin(ax+y)*L
=-0.5*A*B*[sin(ax+ax+y)-cos(ax-ax-y)]*L
=-0.5*A*B*[sin(2ax+y)-cos(-y)]*L
filtering the frequency components by a filter to obtain an I path direct current voltage signal:
VdcI=0.5*A*B*L*cos(y);
further, the specific formula of the generated Q paths of intermediate frequency signals is as follows:
Asin(ax)*Bcos(ax+y)*L
=0.5*A*B*[sin(ax+ax+y)+sin(ax-ax-y)]*L
=0.5*A*B*[sin(2ax+y)+sin(-y)]*L
after the frequency components are filtered by the filter, the Q paths of direct current voltage signals are obtained:
VdcQ=-0.5*A*B*L*sin(y)
further, as long as the phase shift of VrefI and VI is not more than 360 degrees, the exact values of VrefI, vrefQ, VI and VQ can be obtained by fitting and iterative table look-up, and the phase shifts are uniformly distributed on two sine wave curves with 90 ° phase difference, the waveform diagram is shown in fig. 2, wherein the abscissa is voltage U (unit: V), and the ordinate is phase
Figure BDA0002142529750000061
(unit: °) the above VdcQ and VdcI are obtained from the relationship between VrefI, vrefQ, VI and VQ, and y is obtained.
Further, let f be the working frequency of the antenna group, c be the speed of light, and in a phase shift of one period, d=y/(2×pi)/f×c×2, i.e. the distance between the antenna group and the measured object is calculated.
Wherein A, B is a function coefficient;
ax is the frequency;
y is the phase shift amount;
l is a mixing attenuation coefficient;
pi is the circumference ratio;
VI is an I-path voltage signal after the measured object moves;
VQ is Q-path voltage signal after the object to be measured moves;
VdcQ is a Q path direct current voltage signal;
VdcI is the I-path dc voltage signal.
In a preferred embodiment, in step S3, the two intermediate frequency signals are filtered.
Specifically, the two paths of intermediate frequency signals are subjected to filtering processing through a filter.
In a preferred embodiment, the mixing method is a zero intermediate frequency quadrature mixing method.
Specifically, the second radio frequency signal is subjected to zero intermediate frequency quadrature mixing operation so as to obtain two intersecting intermediate frequency signals.
In a preferred embodiment, in step S3, the two intermediate frequency signals are an I intermediate frequency signal and a Q intermediate frequency signal, respectively.
In a preferred embodiment, in step S4, the I-path intermediate frequency signal and the Q-path intermediate frequency signal are used to collect an I-path dc voltage signal and a Q-path dc voltage signal, respectively.
In a preferred embodiment, the first radio frequency signal generates a 24GHz millimeter wave signal.
Specifically, the electromagnetic wave generated by the first radio frequency signal emitted by the antenna group is 24-24.25 GHz millimeter wave, preferably 24.125GHz millimeter wave.
The technical scheme of the invention has the beneficial effects that: the distance measuring method for 24GHz millimeter waves can measure the target distance of a shorter distance (less than 60 cm), can achieve the distance measuring precision of + -1mm, does not need a complex processing process, correspondingly reduces the requirements of software and hardware, reduces the cost and is suitable for popularization.
The foregoing description is only illustrative of the preferred embodiments of the present invention and is not to be construed as limiting the scope of the invention, and it will be appreciated by those skilled in the art that equivalent substitutions and obvious variations may be made using the description and illustrations of the present invention, and are intended to be included within the scope of the present invention.

Claims (6)

1. A ranging method for 24GHz millimeter waves, the ranging method comprising the steps of:
step S1, transmitting a first radio frequency signal through an antenna group;
s2, receiving a second radio frequency signal formed by reflecting the first radio frequency signal through the antenna group;
s3, forming two paths of intermediate frequency signals by the first radio frequency signal and the second radio frequency signal through a frequency mixing method;
s4, collecting two paths of voltage signals through the two paths of intermediate frequency signals;
s5, analyzing the two paths of voltage signals to obtain the distance information between the antenna group and a measured object;
in the step S3, the two intermediate frequency signals are an I intermediate frequency signal and a Q intermediate frequency signal respectively;
the antenna group needs to perform environmental calibration at the beginning of measurement, and the distance of the measured object is fixed to obtain reference voltage signals VrefI and VrefQ of an I path direct current voltage signal and a Q path direct current voltage signal when the measured object is not present, wherein VrefI is an I-path reference voltage signal and VrefQ is a Q-path reference voltage signal, and the reference voltage signals VrefI and VrefQ are taken as subsequent calculation calibration bases;
the method for obtaining the distance information between the antenna group and the measured object comprises the following steps:
if the moving distance of the measured object is D, D is the measured distance, the I path voltage signal acquired after the measured object moves is VI, and the Q path voltage signal is VQ;
the first radio frequency signal is expressed as ftx=asin (ax), and the second radio frequency signal reflected by the measured object is expressed as frx=bsin (ax+y);
mixing the first radio frequency signal and the second radio frequency signal to generate an I path intermediate frequency signal and a Q path intermediate frequency signal, wherein the specific formula of the I path intermediate frequency signal is as follows:
Asin(ax)*Bsin(ax+y)*L;
=-0.5*A*B*[sin(ax+ax+y)-cos(ax-ax-y)]*L;
=-0.5*A*B*[sin(2ax+y)-cos(-y)]*L;
filtering the frequency components by a filter to obtain an I path direct current voltage signal:
VdcI=0.5*A*B*L*cos(y);
the specific formula of the generated Q paths of intermediate frequency signals is as follows:
Asin(ax)*Bcos(ax+y)*L;
=0.5*A*B*[sin(ax+ax+y)+sin(ax-ax-y)]*L;
=0.5*A*B*[sin(2ax+y)+sin(-y)]*L;
filtering the frequency components by a filter to obtain Q paths of direct current voltage signals:
VdcQ=-0.5*A*B*L*sin(y);
when the phase shift of Vrefi and VI is not more than 360 degrees, the exact values of VrefI, vrefQ, VI and VQ are obtained by means of curve fitting and iterative table lookup, and are distributed on two sine wave curves with the phase difference of 90 degrees, so that VdcQ and VdcI are obtained through the relation between VrefI, vrefQ, VI and VQ, and y is further obtained;
let f be the working frequency of the antenna group, c be the speed of light, d=y/(2×pi)/f×c×2 in the phase shift of one period, i.e. calculate the distance between the antenna group and the measured object;
wherein:
a is used to represent the amplitude of the first radio frequency signal;
b is used to represent the amplitude of the second radio frequency signal;
ax is the frequency;
y is the phase shift amount;
l is a mixing attenuation coefficient;
pi is the circumference ratio;
VI is an I-path voltage signal after the measured object moves;
VQ is Q-path voltage signal after the object to be measured moves;
VdcQ is a Q path direct current voltage signal;
VdcI is the I-path dc voltage signal.
2. The ranging method for 24GHz millimeter waves according to claim 1, wherein in the step S3, the two intermediate frequency signals are filtered.
3. The ranging method for 24GHz millimeter waves according to claim 1, wherein the mixing method is a zero intermediate frequency quadrature mixing method.
4. The method according to claim 1, wherein in the step S4, the I-path intermediate frequency signal and the Q-path intermediate frequency signal are used to collect an I-path direct current voltage signal and a Q-path direct current voltage signal, respectively.
5. The method according to claim 4, wherein in the step S5, the frequencies and phases of the I-path dc voltage signal and the Q-path dc voltage signal are analyzed to calculate the distance information between the antenna group and the measured object.
6. The method of claim 1, wherein the first radio frequency signal generates the 24GHz millimeter wave signal.
CN201910673702.9A 2019-07-24 2019-07-24 Ranging method for 24GHz millimeter waves Active CN110426700B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910673702.9A CN110426700B (en) 2019-07-24 2019-07-24 Ranging method for 24GHz millimeter waves

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910673702.9A CN110426700B (en) 2019-07-24 2019-07-24 Ranging method for 24GHz millimeter waves

Publications (2)

Publication Number Publication Date
CN110426700A CN110426700A (en) 2019-11-08
CN110426700B true CN110426700B (en) 2023-06-23

Family

ID=68412278

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910673702.9A Active CN110426700B (en) 2019-07-24 2019-07-24 Ranging method for 24GHz millimeter waves

Country Status (1)

Country Link
CN (1) CN110426700B (en)

Citations (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0010064A1 (en) * 1978-10-11 1980-04-16 KERN & CO. AG Werke für Präzisionsmechanik Optik und Elektronik Method of electro-optical distance measurement and apparatus for carrying out the method
US5325095A (en) * 1992-07-14 1994-06-28 The United States Of America As Represented By The United States Department Of Energy Stepped frequency ground penetrating radar
JP2000338233A (en) * 1999-05-28 2000-12-08 Mitsubishi Electric Corp Pulse doppler radar device
CN102012507A (en) * 2009-09-07 2011-04-13 阿尔卑斯电气株式会社 Wireless sensor device
CN202119902U (en) * 2011-06-24 2012-01-18 北京理工大学 77 GHz millimeter wave automobile anti-collision radar signal processing device
CN102328751A (en) * 2011-08-04 2012-01-25 南京航空航天大学 System for assisting airport runway perambulation inspection
GB201315114D0 (en) * 2013-08-23 2013-10-09 Agd Systems Ltd Radar apparatus and method
CN104914453A (en) * 2015-05-13 2015-09-16 北京理工大学 Carrier-phase-based multi-channel pseudorange measuring device and method
DE102017211558A1 (en) * 2016-07-07 2018-01-11 Infineon Technologies Ag RADAR SYSTEMS AND RELATED METHODS
CN107783107A (en) * 2016-08-25 2018-03-09 大连楼兰科技股份有限公司 The millimetre-wave radar altimeter of plant protection rotor wing unmanned aerial vehicle
CN207867029U (en) * 2018-03-01 2018-09-14 杭州睿达汽车科技有限公司 A kind of signal transmitting and receiving module for 24G high-precision ranging radars
CN109373942A (en) * 2018-10-12 2019-02-22 北京理工大学 A kind of phase acquisition methods in tip clearance measuring system based on Vivado HLS
CN109617633A (en) * 2018-12-19 2019-04-12 北京无线电计量测试研究所 A kind of Attenuation measuring system and method

Patent Citations (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0010064A1 (en) * 1978-10-11 1980-04-16 KERN & CO. AG Werke für Präzisionsmechanik Optik und Elektronik Method of electro-optical distance measurement and apparatus for carrying out the method
US5325095A (en) * 1992-07-14 1994-06-28 The United States Of America As Represented By The United States Department Of Energy Stepped frequency ground penetrating radar
JP2000338233A (en) * 1999-05-28 2000-12-08 Mitsubishi Electric Corp Pulse doppler radar device
CN102012507A (en) * 2009-09-07 2011-04-13 阿尔卑斯电气株式会社 Wireless sensor device
CN202119902U (en) * 2011-06-24 2012-01-18 北京理工大学 77 GHz millimeter wave automobile anti-collision radar signal processing device
CN102328751A (en) * 2011-08-04 2012-01-25 南京航空航天大学 System for assisting airport runway perambulation inspection
GB201315114D0 (en) * 2013-08-23 2013-10-09 Agd Systems Ltd Radar apparatus and method
CN104914453A (en) * 2015-05-13 2015-09-16 北京理工大学 Carrier-phase-based multi-channel pseudorange measuring device and method
DE102017211558A1 (en) * 2016-07-07 2018-01-11 Infineon Technologies Ag RADAR SYSTEMS AND RELATED METHODS
CN107783107A (en) * 2016-08-25 2018-03-09 大连楼兰科技股份有限公司 The millimetre-wave radar altimeter of plant protection rotor wing unmanned aerial vehicle
CN207867029U (en) * 2018-03-01 2018-09-14 杭州睿达汽车科技有限公司 A kind of signal transmitting and receiving module for 24G high-precision ranging radars
CN109373942A (en) * 2018-10-12 2019-02-22 北京理工大学 A kind of phase acquisition methods in tip clearance measuring system based on Vivado HLS
CN109617633A (en) * 2018-12-19 2019-04-12 北京无线电计量测试研究所 A kind of Attenuation measuring system and method

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
双通道连续波多普勒雷达测速模型仿真;刘邹;《计算机仿真》;20181130;全文 *
应用欠采样原理提高相位式激光测距精度;孙懋珩等;《红外与激光工程》;20090225(第01期);全文 *
毫米波主动探测系统的信号处理算法及实现;孙峰;《中国优秀硕士学位论文全文数据库信息科技辑》;20170715;I136-311 *

Also Published As

Publication number Publication date
CN110426700A (en) 2019-11-08

Similar Documents

Publication Publication Date Title
US11209468B2 (en) Apparatus and method for detecting object features
CN105306053A (en) Digital PLL (Phase-Locked Loop) based phase noise measuring device and method
CN104122444B (en) All-digital IF spectrum analyzer and frequency spectrum analysis method
KR102169078B1 (en) Measuring method and measuring device for measuring broadband measurement signals
CN205749892U (en) A kind of high accuracy based on microwave interferometer surveys ship radar
CN210742490U (en) Intermediate frequency analog circuit of continuous wave radar, continuous wave radar and movable platform
CN113433540B (en) Phase difference detection equipment for FMCW modulation
CN110426700B (en) Ranging method for 24GHz millimeter waves
US11041939B2 (en) Signal demodulation device having IQ mixer and demodulation method using the same
CN106569046A (en) Improved intermediate frequency delay line frequency discrimination method-based phase noise test device and method
CN106841824B (en) Signal source comprehensive parameter on-site measuring device
Boukari et al. A heterodyne six-port FMCW radar sensor architecture based on beat signal phase slope techniques
CN113405579B (en) Microwave sensor detection circuit for multiple detection scenes and design method thereof
Kaminski et al. K-band FMCW radar module with interferometic capability for industrial applications
Yu et al. An indoor S-band radar receive array testbed
KR101766765B1 (en) System for Linear Phase shift Type Reflectometer
KR101358904B1 (en) Amplitude modulated radar, apparatus and method for reducing a distance measurement error of the same
CN206114773U (en) High performance spectral analyser
RU2661488C1 (en) Method of the distance measurement
CN111638490B (en) FMCW transmitting circuit and method with invariable bandwidth center frequency capable of continuously changing
CN108196237A (en) A kind of method for inhibiting parastic modulation in fmcw radar echo-signal
CN113567947A (en) Demodulation method of Doppler phase shift signal
CN110476057B (en) Flow measurement system
Yang et al. Beat Signal Analysis for Terahertz Frequency Modulation Continuous Wave
SU1045148A2 (en) Digital panoramic frequency meter

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
CP03 Change of name, title or address
CP03 Change of name, title or address

Address after: No. 0459, Unit 209, No. 62 Chengyi North Street, Software Park Phase III, Torch High tech Zone, Xiamen City, Fujian Province, 361000

Patentee after: Sijie Microelectronics (Xiamen) Co.,Ltd.

Address before: 201800 room j461, building 6, 1288 Yecheng Road, Jiading District, Shanghai

Patentee before: SHANGHAI SILICON MICROELECTRONICS Co.,Ltd.