WO2013037217A1 - Method and apparatus for acquiring standing wave ratio - Google Patents

Method and apparatus for acquiring standing wave ratio Download PDF

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Publication number
WO2013037217A1
WO2013037217A1 PCT/CN2012/076044 CN2012076044W WO2013037217A1 WO 2013037217 A1 WO2013037217 A1 WO 2013037217A1 CN 2012076044 W CN2012076044 W CN 2012076044W WO 2013037217 A1 WO2013037217 A1 WO 2013037217A1
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Prior art keywords
vector
signal
values
value
standing wave
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PCT/CN2012/076044
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French (fr)
Chinese (zh)
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李凡龙
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中兴通讯股份有限公司
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Publication of WO2013037217A1 publication Critical patent/WO2013037217A1/en

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    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B17/00Monitoring; Testing
    • H04B17/30Monitoring; Testing of propagation channels
    • H04B17/391Modelling the propagation channel

Definitions

  • the present invention relates to the field of communications, and in particular to a method and apparatus for acquiring a standing wave ratio.
  • the standing wave ratio is used to measure impedance matching in a signal transmission link.
  • the standing wave ratio is defined by the magnitude of the reflection coefficient. The details are as follows: Assuming that the forward wave (also called the transmitted wave) is ⁇ , the reflected wave, the coefficient of the reflection is defined as: It should be noted that ⁇ is a complex vector that describes the amplitude and phase of the reflection. According to the definition of standing wave ratio:
  • the standing wave ratio is a value greater than 1, and the larger the standing wave ratio, the larger the reflected signal is, and the worse the matching of the signal transmission is.
  • the traditional method of standing wave ratio detection is to calculate the return loss by obtaining the reflected power and the incident power of the signal, and finally calculate the standing wave ratio. This method is called scalar detection. The method is based on the definition of the standing wave ratio. If it is necessary to know the standing wave ratio, the amplitude of the reflection coefficient needs to be obtained, and the conversion is expressed in the form of power, and the return wave loss is further derived by using the return loss. That is, using the conversion relationship between amplitude and power, the expression of the standing wave ratio is re-introduced, which is briefly explained below:
  • RL ⁇ 0Log ⁇ - Return Loss (RL for short) is defined as: ... (4); Combining the above formulas (3) and (4), we can obtain: ( 5 ); Therefore, the scalar detection method of the standing wave ratio calculates the return loss by acquiring the reflected power and the incident power of the signal. Finally, the standing wave ratio is calculated. This method is widely applied to communication systems. However, if you want to ensure the rationality of the above-mentioned standing wave ratio scalar detection method and the accuracy of the obtained standing wave ratio, you need to make the following conditions for the system and its measurement:
  • the acquisition points of the incident signal and the reflected signal must all come from the point where the matching condition expressed by the standing wave ratio is desired. That is, when it is necessary to detect the standing wave ratio indicating that the point A is matched, the detection point is placed at point B different from the point A.
  • the detection path through which the incident and reflected signal power is detected must have exactly the same gain characteristics, which are generally measured in terms of amplitude and phase.
  • FIG. 1 is a schematic diagram of the standing wave ratio detection in the RRU in the wireless communication according to the related art, below The detection of the standing wave ratio will be described with reference to FIG. As shown in FIG.
  • the signal 1 is a transmission signal (Forward, referred to as FWD, also becomes an incident signal), and the signal 5 is a reflection signal (Reverse, abbreviated as REV).
  • FWD Forward
  • REV Reflective
  • the existing scalar detection method results in low accuracy of standing wave ratio detection. In practical applications, it is difficult to obtain a detection value of a higher precision standing wave ratio.
  • the present invention provides a method and apparatus for acquiring a standing wave ratio, which at least solves the problem of low accuracy and inaccuracy of standing wave ratio detection of the above-described conventional scalar standing wave ratio detecting method.
  • a method for acquiring a standing wave ratio comprising: respectively acquiring a vector representation of physical property values of an incident signal and a reflected signal; and abstracting the standing wave ratio detecting device into a vector model,
  • the parameter value of the physical expression corresponding to the vector model includes a physical attribute value of the incident signal represented by a vector and a physical attribute value of the reflected signal, and the value of the expression corresponding to the vector model is a reflection coefficient, wherein The reflection coefficient is a vector value; and the standing wave ratio is obtained according to the reflection coefficient.
  • obtaining a vector representation of the physical property values of the incident signal and the reflected signal respectively comprises: obtaining a vector representation of the physical property values of the incident signal and the reflected signal by measurement, respectively.
  • respectively obtaining a vector representation of the physical property values of the incident signal and the reflected signal comprises: respectively obtaining two different types of scalar values of the incident signal and the reflected signal by measurement, according to the different types of scalar values Obtaining a vector representation of physical property values of the incident signal and the reflected signal.
  • the two different types of scalar values are power values and phase values.
  • obtaining the constant value in the vector model comprises: acquiring a vector value of the physical property value of the fixed incident signal and the reflected signal respectively corresponding to the plurality of sets of known fixed loads obtained by using the standing wave ratio detecting device;
  • the standing wave ratio detecting means respectively corresponds to a vector value of a physical value of a fixed incident signal and a reflected signal in the case of an open circuit, a short circuit and a perfect match; and according to the reflection coefficient and the incident signal and the reflection The vector value of the physical property value of the signal results in a constant value in the vector model.
  • obtaining the constant value in the vector model comprises: obtaining an amplitude of the reflection coefficient according to the measured power value of the incident signal and the reflected signal, and the incident signal and the reflected signal according to the measurement
  • the phase value obtains a phase value of the reflection coefficient
  • a constant value in the vector model is obtained according to a vector value of the plurality of sets of the reflection coefficient and a vector value of the incident signal and a physical property value of the reflected signal.
  • a standing wave ratio obtaining apparatus comprising: a first acquiring module configured to respectively acquire a vector representation of physical property values of an incident signal and a reflected signal; an abstract module, setting In order to abstract the standing wave ratio detecting device into a vector model, the parameter values of the physical expression corresponding to the vector model include a physical attribute value of the incident signal represented by a vector and a physical attribute value of the reflected signal, The value of the expression corresponding to the vector model is a reflection coefficient, wherein the reflection coefficient is a vector value; and the second acquisition module is configured to acquire the standing wave ratio according to the reflection coefficient.
  • the first acquiring module is configured to acquire the vector representation by at least one of: obtaining a vector representation of physical property values of the incident signal and the reflected signal by measurement; respectively, obtaining the incident by measurement
  • Two different types of scalar values of the signal and the reflected signal, a vector representation of the physical property values of the incident signal and the reflected signal is obtained from the different types of scalar values.
  • the two different types of scalar values are power values and phase values.
  • the abstraction module is configured to acquire a constant value in the vector model according to at least one of the following: obtaining the transmission parameter respectively corresponding to a fixed set of fixed fixed loads obtained by using the standing wave ratio detecting device a vector value of a physical property value of the signal and the reflected signal, for example, the standing wave ratio detecting means respectively corresponds to a vector value of a physical value of the fixed incident signal and the reflected signal in the case of an open circuit, a short circuit, and a perfect match; a reflection coefficient and a vector value of a physical property value of the incident signal and the reflected signal to obtain a constant value in the vector model; acquiring the power value according to the measured incident signal and the reflected signal a magnitude of the reflection coefficient, the phase value of the reflection coefficient is obtained according to the measured phase value of the incident signal and the reflected signal; and the vector value of the plurality of sets of the reflection coefficient and the incident signal and the reflected signal The vector value of the physical property value yields a constant value in the vector model.
  • the vector detection method is adopted, and the standing wave ratio detecting device is abstracted into a vector model without using the condition limitation, and the reflection coefficient is obtained by using the expression corresponding to the vector model, and the standing wave is obtained. Therefore, the conditional limitation of the standing wave ratio scalar detection method to the standing wave ratio detection system is eliminated, and the problem of low standing wave ratio detection accuracy of the existing scalar standing wave ratio detection method is solved, and the problem of inaccuracy is effectively improved, and the station is effectively improved. The detection accuracy of the wave ratio.
  • FIG. 1 is a schematic diagram of standing wave ratio detection in an RRU in wireless communication according to the related art
  • FIG. 2 is a flowchart of a standing wave ratio acquisition method according to an embodiment of the present invention
  • 4 is a schematic diagram of a standing wave ratio detecting device in a wireless system according to the related art
  • FIG. 1 is a schematic diagram of standing wave ratio detection in an RRU in wireless communication according to the related art
  • FIG. 2 is a flowchart of a standing wave ratio acquisition method according to an embodiment of the present invention
  • FIG. A block diagram of a configuration of a standing wave ratio acquisition device
  • 4 is a schematic diagram of a standing wave ratio detecting device in a wireless system according to the related art
  • FIG. 5 is a schematic diagram of an abstract vector model of a standing wave ratio detecting device in a wireless system according to a limited embodiment of the present invention
  • FIG. 6 is a preferred embodiment according to the present invention.
  • FIG. 7 is a flowchart of a method for acquiring a loop delay according to a preferred embodiment of the present invention
  • FIG. 8 is a reflection coefficient 1 ⁇ according to a preferred embodiment of the present invention
  • FIG. 9 is a flowchart of a method for acquiring the amplitude of a channel independent reflection coefficient according to a preferred embodiment of the present invention
  • FIG. 10 is a reflection coefficient of channel multiplexing according to a preferred embodiment of the present invention.
  • FIG. 2 is a flowchart of a VSWR acquisition method according to an embodiment of the present invention.
  • the method includes the following steps: Step S202: Acquire a vector representation of physical property values of an incident signal and a reflected signal, respectively.
  • Step S204 abstracting the standing wave ratio detecting device into a vector model, and the parameter values of the physical expression corresponding to the vector model include physical property values of the incident signal represented by the vector and physical property values of the reflected signal, and expressions corresponding to the vector model
  • the value is the reflection coefficient, where the reflection coefficient is a vector value.
  • Step S206 obtaining a standing wave ratio according to the reflection coefficient.
  • the vector detection method is adopted, and the reflection coefficient is obtained by abstracting the standing wave ratio detecting device into a vector model without using the condition limitation, and using the expression corresponding to the vector model.
  • the standing wave ratio is obtained, thereby eliminating the conditional limitation of the standing wave ratio scalar detecting method on the standing wave ratio detecting system, and solving the problem that the existing scalar standing wave ratio detecting method has low accuracy and inaccuracy of standing wave ratio detection, and The detection accuracy of the standing wave ratio is effectively improved.
  • the manner of obtaining the vector representation of the physical attribute values of the incident signal and the reflected signal may include a plurality of types, which may be selected according to actual needs.
  • the measuring device can measure the vector
  • the vector measuring device can be used to obtain a vector representation of the physical property values of the incident signal and the reflected signal, respectively. This way of obtaining is simple.
  • the scalar measuring device can be used to respectively obtain two different types of scalar values of the incident signal and the reflected signal, and then obtain according to different types of scalar values.
  • the medium acquisition method can obtain a vector representation of physical property values of the incident signal and the reflected signal on the basis of the existing scalar measuring device, and is relatively common.
  • the above two methods can be used alone or in combination with each other to obtain a vector representation of the physical property values of the incident signal and the reflected signal.
  • two different types of scalar values are power values and phase values.
  • the corresponding expression contains constant parameters.
  • there may be different numbers of constant values for example, three
  • three sets of reflection coefficients and incident signals and reflections are required.
  • the vector value of the physical property value of the signal constitutes three ways to calculate three different constants. That is, the number of equations corresponding to the number of constants can be constructed.
  • the method for obtaining the constant parameters in the expression can include a plurality of types, and can be selected according to actual needs.
  • a plurality of sets of known fixed loads obtained by using the standing wave ratio detecting means may respectively obtain vector values of physical property values of the fixed incident signal and the reflected signal by acquiring the reflection coefficient, for example, the standing wave ratio detecting means is open, In the case of short circuit and perfect match, respectively, corresponding to the vector values of the physical values of the fixed incident signal and the reflected signal; respectively, and then the constant values in the vector model are obtained from the reflection coefficient and the vector value of the physical property values of the incident signal and the reflected signal. .
  • This way of obtaining through the special values corresponding to the three special cases is general.
  • the amplitude of the reflection coefficient is obtained according to the measured power values of the incident signal and the reflected signal
  • the phase value of the reflection coefficient is obtained according to the measured phase values of the incident signal and the reflected signal
  • the vector values according to the plurality of sets of reflection coefficients and The vector values of the physical property values of the incident and reflected signals result in constant values in the vector model.
  • This method is suitable when the device that measures the data can only measure the scalar.
  • the above methods can be used alone or in combination with each other to obtain constant parameter values in the expression.
  • a standing wave ratio obtaining device is further provided, which is used to implement the above embodiments and preferred embodiments thereof, and has not been described again, and the following relates to the device.
  • module may implement a combination of software and/or hardware of a predetermined function.
  • the systems and methods described in the following embodiments are preferably implemented in software, hardware, or a combination of software and hardware, is also possible and contemplated.
  • 3 is a structural block diagram of a standing wave ratio acquisition apparatus according to an embodiment of the present invention. As shown in FIG. 3, the apparatus includes a first acquisition module 30, an abstraction module 32, and a second acquisition module 34. The module and its functions are described.
  • the first obtaining module 30 is configured to respectively obtain vector representations of physical attribute values of the incident signal and the reflected signal; the abstract module 32 is coupled to the first obtaining module 30, and the abstracting module 32 is configured to abstract the standing wave ratio detecting device into a vector
  • the parameter value of the physical expression corresponding to the model, the physical value of the incident signal represented by the vector and the physical property value of the reflected signal, and the value of the expression corresponding to the vector model is a reflection coefficient, wherein the reflection coefficient is a vector
  • the second acquisition module 34 is coupled to the abstraction module 32, which is arranged to acquire the standing wave ratio based on the reflection coefficient.
  • the first obtaining module 30 is configured to obtain a vector representation in a plurality of manners, for example, a vector representation of physical property values of the incident signal and the reflected signal respectively by measurement; and, for example, respectively, the incident signal is obtained by measurement
  • Two different types of scalar values of the reflected signal, according to different types of scalar values to obtain a vector representation of the physical property values of the incident signal and the reflected signal preferably, two different types of scalar values are power values And phase values.
  • the above two acquisition methods may be applied separately or in combination with each other to obtain a vector representation.
  • the abstraction module 32 can obtain the constant values in the vector model in a plurality of different manners, for example, acquiring the transmission parameters in the plurality of sets of known fixed loads obtained by using the standing wave ratio detecting means respectively corresponding to the fixed incident and reflected signals.
  • a vector value of a physical attribute value for example, the standing wave ratio detecting means respectively corresponds to a vector value of a physical value of a fixed incident signal and a reflected signal in the case of an open circuit, a short circuit, and a perfect match; according to the reflection coefficient and the incident signal and the reflection
  • the vector value of the physical property value of the signal is obtained as a constant value in the vector model; for example, the amplitude of the reflection coefficient is obtained according to the measured power value of the incident signal and the reflected signal, and the phase of the incident signal and the reflected signal are obtained according to the measurement.
  • the value obtains the phase value of the reflection coefficient; the vector value according to the plurality of sets of reflection coefficients And the vector values of the physical property values of the incident signal and the reflected signal are obtained as constant values in the vector model.
  • the above two acquisition methods may be applied separately or in combination with each other to obtain a constant value in the vector model.
  • the following is a description of a preferred embodiment in combination with the above-described embodiments and preferred embodiments thereof.
  • the standing wave ratio scalar detection method is eliminated by a standing wave ratio vector detection method.
  • the ratio detecting device is abstracted into a vector model, which can be abstracted into different vector models according to components of the standing wave ratio detecting device and their ports, for example, may be a dual port vector model, a three-port vector model, etc., thereby eliminating the pair
  • the condition of the standing wave ratio detection system is limited, thereby improving the detection accuracy of the standing wave ratio.
  • a standing wave ratio vector detecting device according to a preferred embodiment of the present invention will be described by taking a standing wave ratio dual port detecting device in a wireless system as an example.
  • 4 is a schematic diagram of a standing wave ratio detecting device in a wireless system according to the related art. As shown in FIG.
  • the device includes a signal source generator (also referred to as a signal source generator) 400, a signal transmitting link 402, and a signal amplifier. 404, coupler 406, filter 408, antenna system (ANT) 410, 2-to-1 switch 412, signal detection link 414, and signal detector 416.
  • the various components of the device and their functions are described below.
  • the signal source generator 400 mainly generates a signal source that needs to be transmitted. It should be noted that it may be from another device or a separate signal generator.
  • the signal transmission link 402 is coupled to the signal source generator 400 and is primarily configured to transmit signals that need to be transmitted, which may be constructed of a number of elements.
  • Signal amplifier 404 is coupled to signal transmission link 402 and is primarily configured to perform amplification processing of the signal.
  • Coupler 406 is coupled to signal amplifier 404 and is primarily configured to couple the transmit and reflected signals for detection.
  • the filter 408 is connected to the coupler 406, and is mainly configured to complete the filtering of the signal to ensure the transmission purity of the signal, and may also be set to perform separation of the transmission and reception.
  • the ANT410 is primarily set to transmit signals.
  • the 2-to-1 switch 412 is coupled to the coupler 406 and the filter 408, and is primarily configured to perform a 2-to-1 function of the transmitted and reflected signals.
  • the signal detection link 414 is connected to the 2-to-1 switch 412, which is primarily configured to complete the reception of the transmitted and reflected signals for easy detection. It can be composed of a number of independent elements.
  • Signal detector 416 is coupled to signal detection link 414, primarily to detect the completion of the signal, and can be any device with automatic processing capabilities (eg, conventional CPUs, DSPs, FPGAs, etc.).
  • the VSWR detection device in the wireless system of FIG. 4 is a vector model. Since the device is a two-port network, no matter how many components of the incident signal and the reflected signal are transmitted and each component is a dual port, the final abstraction is A dual port S-parameter model is used to represent.
  • 5 is a schematic diagram of an abstract vector model of a standing wave ratio detecting device in a wireless system according to a limited embodiment of the present invention. As shown in FIG. 5, the vector model of the dual port will be described. As shown in FIG. 5, V TMD is a transmission signal, V « ⁇ is a reflection signal, and S11, S12, S21, and S22 are parameters of the model. According to the vector model, an expression of the reflection coefficient can be accurately obtained as follows: Oh,
  • Method 1 Obtain a reflection coefficient corresponding to a vector value in the case where the standing wave ratio detecting device is open, short, and fully matched, wherein the open circuit, the short circuit, and the perfect match respectively correspond to the physical values of the fixed incident signal and the reflected signal.
  • Vector value a constant value in the vector model is obtained from the reflection coefficient and the vector value of the physical property values of the incident signal and the reflected signal. Step one can be calculated in real time by using the method of solving the phase and amplitude in the second method.
  • Step 2 The three unknowns can be obtained by using 1 ⁇ for three known cases without loss of generality.
  • three special cases are used, namely open circuit, short circuit and matching to obtain three equations.
  • the 1 ⁇ 1 corresponding to these three cases is divided into three values of 0, -1 and 1, and the phases correspond to 0, 180 and 0, respectively.
  • ⁇ - ⁇ can be calculated separately, where '"- ⁇ ' is the value of the matching case, '"-°, which is the value of the open circuit case, in the case of short circuit
  • the resulting reflection coefficient is also a vector value, and all quantities in equation (7) are vectors, and any vector has amplitude and phase information. Thereby the standing wave ratio is accurately obtained.
  • Method 2 obtaining the amplitude of the reflection coefficient according to the measured power values of the incident signal and the reflected signal, and obtaining the phase value of the reflection coefficient according to the measured phase values of the incident signal and the reflected signal; and the vector values according to the plurality of sets of reflection coefficients and The vector values of the physical property values of the incident and reflected signals result in constant values in the vector model. This method is suitable when the device that measures the data can only measure the scalar.
  • FIG. 6 is a schematic diagram of an abstracted reflected signal detection path and an incident signal detection path according to a preferred embodiment of the present invention.
  • the components can always be abstracted into a reflected signal detection path and an incident signal detection path.
  • FIG. 7 is a flowchart of a method for acquiring a loop delay according to a preferred embodiment of the present invention. As shown in FIG. 7, the method includes the following steps: Step S702, turning on a signal source generator. Step S704, simultaneously acquiring the signal ⁇ generated by the signal source and the transmitted incident signal FWD. Step S706, correlating the TX signal and the FWD signal to obtain a correlation peak. In step S708, it is determined whether or not there is a correlation peak. If the determination is yes, the process goes to step S712.
  • FIG. 8 is a flowchart of a method for acquiring a phase of a reflection coefficient 1 ⁇ according to a preferred embodiment of the present invention. As shown in FIG. 8, the method includes the following steps: Step S802: determining whether a signal transmitter has a signal, and determining a result If it is no, it is directly terminated.
  • step S804 is executed.
  • the RF switch is selected to the FWD, and the TX and FWD data of the same length are simultaneously collected and saved while ensuring the start of the acquisition of the signal source TX signal and the start of the acquisition of the transmission signal FWD.
  • the RF switch is selected to the REV, and the TX and REV data of the same length are simultaneously acquired and saved in the case of ensuring the start of the acquisition of the signal source TX signal and the start of the acquisition of the reflected signal REV.
  • Step S808 Calculate the sliding correlation process by using the collected TX and FWD data, find the correlation peak, and perform data alignment processing to determine the phase change of the FWD relative to the TX.
  • Step S810 calculating, by using the collected TX and REV data, performing a sliding correlation process, and after finding the correlation peak, performing data alignment processing to obtain a change value of the phase of the REV relative to the TX.
  • the detection channels of FWD and REV are independent, then a piece of data of TX0 and REVO at the time of TO is simultaneously acquired while acquiring the forward data, and then the phase change of REVO with respect to TX0 can be calculated by the relevant alignment process.
  • the amount ⁇ Q if the detection channels of FWD and REV are independent, then a piece of data of TX0 and REVO at the time of TO is simultaneously acquired while acquiring the forward data, and then the phase change of REVO with respect to TX0 can be calculated by the relevant alignment process.
  • the amount ⁇ Q if the detection channels of FWD and REV are independent, then a piece of data of TX0 and REVO at the time of TO is simultaneously acquired while acquiring the forward data, and then the phase change of REVO with respect to TX
  • the purpose of ensuring that the link has no phase fluctuation during this period of time is within the time interval of the second generation after the completion of the forward acquisition. For example, at the time T1, a piece of data of TX1 and REV1 is simultaneously acquired, and the phase change amount ⁇ 1 of REV1 with respect to TX1 can also be obtained. Step S812, using the phase difference value of the REV relative to the TX minus the phase difference value of the FWD relative to the TX
  • FIG. 9 is a flowchart of a method for acquiring the amplitude of a channel independent reflection coefficient ⁇ according to a preferred embodiment of the present invention. As shown in FIG.
  • Step S902 determining whether a signal transmitter has a signal, If the result of the determination is negative, the process is directly terminated. If the determination is YES, step S904 is executed.
  • step S904 the RF switch is selected to the FWD, and the TX and FWD data of the same length are simultaneously acquired and saved while ensuring the start of the acquisition of the signal source TX signal and the start of the acquisition of the transmission signal FWD.
  • step S906 the RF switch is selected to the REV, and the TX and REV data of the same length are simultaneously acquired and saved in the case of ensuring the start of the acquisition of the signal source TX signal and the start of the acquisition of the reflected signal REV.
  • Step S908 directly calculating the average power of the incident signal according to the measured data and the calculation formula of the average power. And the average power of the reflected signal. .
  • FIG. 10 is a flowchart of a method for acquiring the amplitude of a reflection coefficient during channel multiplexing according to a preferred embodiment of the present invention. As shown in FIG. 10, the method includes the following steps: Step S1002: determining whether a signal transmitter has a signal, If the result of the determination is negative, the process is directly terminated. If the determination is YES, step S1004 is executed. In step S1004, the RF switch is selected to the FWD, and the delay of the acquisition of the signal source TX and the start of the acquisition of the transmission signal FWD are simultaneously acquired as the loop delay, and the same length data of the TX and the FWD are simultaneously collected and saved.
  • the correlation alignment can accurately obtain the delay of the link of the forward signal TX and the link of the transmission signal detection point.
  • the RF switch is selected to the REV, and the delay of the start of the acquisition of the signal source TX and the start of the acquisition of the reflected signal REV is the same as the loop delay, and the same length data of the TX and the REV are simultaneously collected and saved, where the power is involved.
  • the power of TX0 is detected at the time of detecting the forward direction, such as the TO time.
  • the reflection and incident signals are detected at a time delay of 7 ⁇ .
  • the ⁇ and REVO data acquired at the same time as the phase ⁇ 0 respectively calculate the power of the segment data, generally the mean power, respectively: P w and 5 « ⁇ . , use ⁇ .
  • Step S1012 using the obtained FWD and REV powers, the amplitude of the reflection coefficient can be calculated, respectively
  • the amplitude of the reflection coefficient can be obtained by using p wdo .
  • a standing wave ratio acquisition software is also provided, which is used to implement the technical solutions described in the above embodiments and preferred embodiments.
  • a storage medium is also provided, the software being stored, including but not limited to an optical disk, a floppy disk, a hard disk, a rewritable memory, and the like.
  • the invention is not limited to any specific combination of hardware and software.
  • the above is only the preferred embodiment of the present invention, and is not intended to limit the present invention, and various modifications and changes can be made to the present invention. Any modifications, equivalent substitutions, improvements, etc. made within the spirit and scope of the present invention are intended to be included within the scope of the present invention.

Abstract

Disclosed are a method and apparatus for acquiring a standing wave ratio. The method comprises: acquiring vector expressions of physical attribute values of an incident signal and a reflected signal respectively; abstracting a standing wave ratio detection apparatus into a vector model, parameter values of a physical expression corresponding to the vector model comprising the physical attribute value of the incident signal and the physical attribute value of the reflected signal which are expressed by using vectors, a value of an expression corresponding to the vector model being a reflection coefficient, and the reflection coefficient is a vector value; and acquiring a standing wave ratio according to the reflection coefficient. The present invention improves the precision of standing wave ratio detection.

Description

驻波比获取方法及装置 技术领域 本发明涉及通信领域, 具体而言, 涉及一种驻波比获取方法及装置。 背景技术 在通信技术中, 驻波比是用于衡量信号传输链路中的阻抗匹配情况的。 驻波比是 用反射系数的幅度来进行定义的, 具体情况如下: 假设前向波 (也称为发射波) 为 ^, 反射波 , 则反射的系数定义为:
Figure imgf000002_0001
需要说明的是, Γ是一个复矢量, 描述了反射的幅度和相位。 按照驻波比的定义得到:
TECHNICAL FIELD The present invention relates to the field of communications, and in particular to a method and apparatus for acquiring a standing wave ratio. BACKGROUND OF THE INVENTION In communication technology, the standing wave ratio is used to measure impedance matching in a signal transmission link. The standing wave ratio is defined by the magnitude of the reflection coefficient. The details are as follows: Assuming that the forward wave (also called the transmitted wave) is ^, the reflected wave, the coefficient of the reflection is defined as:
Figure imgf000002_0001
It should be noted that Γ is a complex vector that describes the amplitude and phase of the reflection. According to the definition of standing wave ratio:
χ -ρ ), 其中, , 即为反射系数的幅度。 按照上述驻波比的定义可知: 驻波比都是大于 1的一个值, 而且驻波比越大, 说 明反射信号越大, 同时也表示信号传输的匹配情况越差。 传统的驻波比检测方法是通过获取反射功率和信号的入射功率,计算出回波损耗, 最后计算出驻波比。 这种方法称之为标量检测法。 该方法是按照驻波比的定义, 如果 需要知道驻波比就需要求出反射系数的幅度, 从而转换为用功率的形式来表示, 并进 一步衍生出用回波损耗来求出驻波比。 即, 利用了幅度和功率之间的转换关系, 重新 推出驻波比的表达式, 下面对其进行简单地说明: χ -ρ ), where , is the magnitude of the reflection coefficient. According to the definition of the above standing wave ratio, the standing wave ratio is a value greater than 1, and the larger the standing wave ratio, the larger the reflected signal is, and the worse the matching of the signal transmission is. The traditional method of standing wave ratio detection is to calculate the return loss by obtaining the reflected power and the incident power of the signal, and finally calculate the standing wave ratio. This method is called scalar detection. The method is based on the definition of the standing wave ratio. If it is necessary to know the standing wave ratio, the amplitude of the reflection coefficient needs to be obtained, and the conversion is expressed in the form of power, and the return wave loss is further derived by using the return loss. That is, using the conversion relationship between amplitude and power, the expression of the standing wave ratio is re-introduced, which is briefly explained below:
按照 的定义, 如果用功率来表示可以表示为:
Figure imgf000002_0002
According to the definition, if expressed by power, it can be expressed as:
Figure imgf000002_0002
RL = \0Log^- 回波损耗 (Return Loss, 简称为 RL) 的定义为: ... ... (4); 综合上述公式 (3 ) 和 (4) 可以得到: ... ... ( 5 ); 因此, 该驻波比的标量检测法是通过获取反射功率和信号的入射功率, 计算出回 波损耗, 最后计算出驻波比。 该方法被大量地应用到通信系统中。 然而, 如果想要保证上述驻波比标量检测方法的合理性和所求出驻波比的精度, 需要对系统及其测量做出如下条件限制: RL = \0Log^- Return Loss (RL for short) is defined as: ... (4); Combining the above formulas (3) and (4), we can obtain: ( 5 ); Therefore, the scalar detection method of the standing wave ratio calculates the return loss by acquiring the reflected power and the incident power of the signal. Finally, the standing wave ratio is calculated. This method is widely applied to communication systems. However, if you want to ensure the rationality of the above-mentioned standing wave ratio scalar detection method and the accuracy of the obtained standing wave ratio, you need to make the following conditions for the system and its measurement:
( 1 ) 入射信号和反射信号的获取点都必须来自希望用驻波比表示的匹配情况的 点。 即不能在需要检测驻波比的表示的是 A点匹配情况时, 检测点放到不同于 A点的 B点。 (1) The acquisition points of the incident signal and the reflected signal must all come from the point where the matching condition expressed by the standing wave ratio is desired. That is, when it is necessary to detect the standing wave ratio indicating that the point A is matched, the detection point is placed at point B different from the point A.
(2) 入射和反射信号功率检测所经过的检测路径必须具有完全相同的增益特性, 该增益特性一般用幅度和相位来衡量。 (2) The detection path through which the incident and reflected signal power is detected must have exactly the same gain characteristics, which are generally measured in terms of amplitude and phase.
(3 )入射信号和反射信号在检测过程中都必须不受到检测链路中任何其它任何信 号的干扰。 只有在上述三种限制条件全部同时满足时, 使用该驻波比标量检测法检测得到的 驻波比才能正确, 才能获得较高的精度。 然而, 在实际的检测系统 (检测装置) 中很 难保证上述三点完全满足。例如,无线通信系统中的无线射频拉远设备(Radio Remote Uint, 简称为 RRU) 中的驻波比的检测, 图 1 是根据相关技术的无线通信中的 RRU 中驻波比检测的示意图, 下面结合图 1对驻波比的检测进行说明。 如图 1所示, 信号 1为发射信号 (Forward, 简称为 FWD, 也成为入射信号), 信 号 5为反射信号 (Reverse, 简称为 REV)。 首先, 在该驻波比的检测过程中, 希望驻 波比反应的点是 RRU和天线系统 ANT。 然而, 入射信号的检测点放到了部件功率放 大器之后, 反射信号的功率检测点放到了部件滤波器 (Filter) 之前, 因此不能满足上 述限制条件的第一条; 其次, FWD和 REV在 2选 1开关前经过了完全不同的路径, 因此不能满足上述限制条件的第二条; 第三, REV的检测同时会受到发射信号 FWD 的串扰信号 2, 系统内部信号 3, Filter的反射干扰信号 4信号的干扰, 因此不能满足 上述限制条件的第三条。 综合上述分析, 现有的标量检测法导致驻波比检测精度低, 在实际应用中, 难以得到较高精度的驻波比的检测值。 发明内容 本发明提供了一种驻波比获取方法及装置, 以至少解决上述现有的标量驻波比检 测法的驻波比检测精度低、 不准确的问题。 根据本发明的一个方面, 提供了一种驻波比获取方法, 该方法包括: 分别获取入 射信号和反射信号的物理属性值的矢量表示式; 将驻波比检测装置抽象为矢量模型, 所述矢量模型对应的物理表达式的参数值包括使用矢量表示的所述入射信号的物理属 性值和所述反射信号的物理属性值, 所述矢量模型对应的表达式的值为反射系数, 其 中, 所述反射系数为矢量值; 根据所述反射系数获取所述驻波比。 优选地, 分别获取入射信号和反射信号的物理属性值的矢量表示形式包括: 分别 通过测量得到所述入射信号和反射信号的物理属性值的矢量表示式。 优选地, 分别获取入射信号和反射信号的物理属性值的矢量表示形式包括: 分别 通过测量得到所述入射信号和反射信号的两种不同类型的标量值, 根据所述不同类型 的标量值获取到所述入射信号和所述反射信号的物理属性值的矢量表示式。 优选地, 所述两种不同类型的标量值为功率值和相位值。 优选地, 获取所述矢量模型中常数值包括: 获取所述反射系数在使用所述驻波比 检测装置得到的多组已知固定负载分别对应固定的入射信号和反射信号的物理属性值 的矢量值, 例如, 该驻波比检测装置在开路、 短路和完全匹配的情况下分别对应固定 的入射信号和反射信号的物理属性值的矢量值; 根据所述反射系数以及所述入射信号 和所述反射信号的物理属性值的矢量值得到所述矢量模型的中的常数值。 优选地, 获取所述矢量模型中常数值包括: 根据测量得到的所述入射信号和所述 反射信号的功率值获取到所述反射系数的幅度, 根据测量得到的所述入射信号和所述 反射信号的相位值得到所述反射系数的相位值; 根据多组所述反射系数的矢量值以及 所述入射信号和所述反射信号的物理属性值的矢量值得到所述矢量模型的中的常数 值。 根据本发明的另一个方面, 还提供了一种驻波比获取装置, 该装置包括: 第一获 取模块, 设置为分别获取入射信号和反射信号的物理属性值的矢量表示式; 抽象模块, 设置为将驻波比检测装置抽象为矢量模型, 所述矢量模型所对应的物理表达式的参数 值包括使用矢量表示的所述入射信号的物理属性值和所述反射信号的物理属性值, 所 述矢量模型对应的表达式的值为反射系数, 其中, 所述反射系数为矢量值; 第二获取 模块, 设置为根据所述反射系数获取所述驻波比。 优选地, 所述第一获取模块设置为通过以下至少之一获取所述矢量表示式: 分别 通过测量得到所述入射信号和反射信号的物理属性值的矢量表示式; 分别通过测量得 到所述入射信号和反射信号的两种不同类型的标量值, 根据所述不同类型的标量值获 取到所述入射信号和所述反射信号的物理属性值的矢量表示式。 优选地, 所述两种不同类型的标量值为功率值和相位值。 优选地, 所述抽象模块设置为根据以下至少之一获取所述矢量模型中常数值: 获 取所述发射参数在使用所述驻波比检测装置得到的多组已知固定负载分别对应固定的 在入射信号和反射信号的物理属性值的矢量值, 例如, 该驻波比检测装置在开路、 短 路和完全匹配的情况下分别对应固定的入射信号和反射信号的物理属性值的矢量值; 根据所述反射系数以及所述入射信号和所述反射信号的物理属性值的矢量值得到所述 矢量模型的中的常数值; 根据测量得到的所述入射信号和所述反射信号的功率值获取 到所述反射系数的幅度, 根据测量得到的所述入射信号和所述反射信号的相位值得到 所述反射系数的相位值; 根据多组所述反射系数的矢量值以及所述入射信号和所述反 射信号的物理属性值的矢量值得到所述矢量模型的中的常数值。 通过本发明, 采用矢量检测的方法, 在无需进行条件限制的情况下, 通过将驻波 比检测装置抽象为一个矢量模型,以及使用该矢量模型对应的表达式获取到反射系数, 并得到驻波比, 从而消除了驻波比标量检测方法对驻波比检测系统的条件限制, 解决 了现有的标量驻波比检测法的驻波比检测精度低, 不准确的问题, 有效地提高了驻波 比的检测精度。 附图说明 此处所说明的附图用来提供对本发明的进一步理解, 构成本申请的一部分, 本发 明的示意性实施例及其说明用于解释本发明, 并不构成对本发明的不当限定。 在附图 中: 图 1是根据相关技术的无线通信中的 RRU中驻波比检测的示意图; 图 2是根据本发明实施例的驻波比获取方法的流程图; 图 3是根据本发明实施例的驻波比获取装置的结构框图; 图 4是根据相关技术的无线系统中驻波比检测装置的示意图; 图 5是根据本发明有限实施例的无线系统中驻波比检测装置的抽象矢量模型示意 图; 图 6是根据本发明优选实施例的抽象得到的反射信号检测路径和入射信号检测路 径的示意图; 图 7是根据本发明优选实施例的获取环路延迟方法的流程图; 图 8是根据本发明优选实施例的反射系数1^的相位的获取方法的流程图; 图 9是根据本发明优选实施例的通道独立时反射系数 的幅度的获取方法的流程 图; 以及 图 10是根据本发明优选实施例的通道复用时反射系数 ^的幅度的获取方法的流 程图。 具体实施方式 下文中将参考附图并结合实施例来详细说明本发明。 需要说明的是, 在不冲突的 情况下, 本申请中的实施例及实施例中的特征可以相互组合。 现有技术中对于需要进行驻波比检测的系统 (例如, 无线通信系统) 而言, 均采 用驻波比标量检测法来进行驻波比的检测, 但是, 由于驻波比标量检测法的使用时, 需要至少三个假设条件才能使用, 但是在实际应用的环境中, 很难同时满足这三个假 设条件, 因此导致获得的驻波比精度低, 不准确。 在本实施例中提供了一种驻波比获取方法, 该方法适需要进行驻波比检测的各个 领域(例如, 无线领域), 图 2是根据本发明实施例的驻波比获取方法的流程图, 如图 2所示, 该方法包括如下步骤: 步骤 S202, 分别获取入射信号和反射信号的物理属性值的矢量表示式。 步骤 S204, 将驻波比检测装置抽象为矢量模型, 矢量模型对应的物理表达式的参 数值包括使用矢量表示的入射信号的物理属性值和反射信号的物理属性值, 矢量模型 对应的表达式的值为反射系数, 其中, 反射系数为矢量值。 步骤 S206, 根据反射系数获取驻波比。 通过本实施例的上述步骤,采用矢量检测的方法,在无需进行条件限制的情况下, 通过将驻波比检测装置抽象为一个矢量模型, 以及使用该矢量模型对应的表达式获取 到反射系数, 并得到驻波比, 从而消除了驻波比标量检测方法对驻波比检测系统的条 件限制, 解决了现有的标量驻波比检测法的驻波比检测精度低, 不准确的问题, 并且 有效地提高了驻波比的检测精度。 对于矢量模型而言, 在现有技术中存在多种的矢量模型, 可以根据不同的需要来 选择不同的矢量模块, 在下文中会结合优选实施例进行说明。 获取入射信号和反射信号的物理属性值的矢量表示形式的方式可以包括多种, 可 以根据实际情况的需要进行选择。 例如, 在测量装置可以测量矢量的情况下, 可以使 用该矢量测量装置分别通过测量得到入射信号和反射信号的物理属性值的矢量表示 式。 这样的获取方式简单。 又例如, 在测量装置只能测量标量的情况下, 可以使用该标量测量装置分别通过 测量得到入射信号和反射信号的两种不同类型的标量值, 然后, 根据不同类型的标量 值获取到入射信号和反射信号的物理属性值的矢量表示式。 该中获取方式可以在现有 的标量测量装置的基础上获得入射信号和反射信号的物理属性值的矢量表示形式, 比 较通用。 当然上述两种方式可以单独使用, 也可以相互结合来共同获得入射信号和反 射信号的物理属性值的矢量表示形式的方式。 较优地, 两种不同类型的标量值为功率值和相位值。 在矢量模型中, 其对应的表达式中含有常量参数, 对于一个矢量模型而言, 其可 能存在不同数量的常数值(例如, 三个), 那么就需要通过三组反射系数和入射信号和 反射信号的物理属性值的矢量值构成三个方式来计算三个不同的常数。 即构造与常数 数量相对应的方程数量即可。 对于表达式中的常量参数的获取方式可以包括多种, 可以根据实际情况的需要进 行选择。 例如, 可以通过获取反射系数在使用驻波比检测装置得到的多组已知固定负 载分别对应固定的入射信号和反射信号的物理属性值的矢量值, 例如, 该驻波比检测 装置在开路、 短路和完全匹配的情况下分别对应固定的入射信号和反射信号的物理属 性值的矢量值; 然后, 根据反射系数以及入射信号和反射信号的物理属性值的矢量值 得到矢量模型的中的常数值。 这种通过三种特殊情况下对应的特殊值来获取的方式具 有一般性。 又例如, 根据测量得到的入射信号和反射信号的功率值获取到反射系数的幅度, 根据测量得到的入射信号和反射信号的相位值得到反射系数的相位值; 根据多组反射 系数的矢量值以及入射信号和反射信号的物理属性值的矢量值得到矢量模型的中的常 数值。 在测量数据的装置只能测量标量的情况下, 这种方式比较适用。 当然上述方式 可以单独使用, 也可以相互结合来获得表达式中的常量参数值。 在本实施例中, 还提供了一种驻波比获取装置, 该装置用于实现上述实施例及其 优选的实施方式, 已经进行过说明的不再赘述, 下面对该对该装置涉及的各个模块进 行说明。 如以下所使用的, 术语"模块"可以实现预定功能的软件和 /或硬件的组合。 尽 管以下实施例所描述的系统和方法较佳地以软件来实现, 但是硬件, 或者软件和硬件 的组合的实现也是可能并被构想的。 图 3是根据本发明实施例的驻波比获取装置的结构框图, 如图 3所示, 该装置包 括第一获取模块 30、 抽象模块 32和第二获取模块 34, 下面对该装置的各个模块及其 功能进行说明。 第一获取模块 30, 设置为分别获取入射信号和反射信号的物理属性值的矢量表示 式; 抽象模块 32连接至第一获取模块 30, 该抽象模块 32设置为将驻波比检测装置抽 象为矢量模型, 矢量模型所对应的物理表达式的参数值包括使用矢量表示的入射信号 的物理属性值和反射信号的物理属性值, 矢量模型对应的表达式的值为反射系数, 其 中, 反射系数为矢量值; 第二获取模块 34连接至抽象模块 32, 该第二获取模块 34设 置为根据反射系数获取驻波比。 较优地, 第一获取模块 30设置为通过多种方式获取矢量表示式, 例如, 分别通过 测量得到入射信号和反射信号的物理属性值的矢量表示式; 又例如, 分别通过测量得 到入射信号和反射信号的两种不同类型的标量值, 根据不同类型的标量值获取到入射 信号和反射信号的物理属性值的矢量表示式, 较优地, 两种不同类型的标量值为功率 值和相位值。 上述两种获取方式可以单独适用也可以相互结合共同获取矢量表示式。 较优地, 抽象模块 32可以多种不同的方式获取矢量模型中常数值, 例如, 获取发 射参数在使用驻波比检测装置得到的多组已知固定负载分别对应固定的在入射信号和 反射信号的物理属性值的矢量值, 例如, 该驻波比检测装置在开路、 短路和完全匹配 的情况下分别对应固定的入射信号和反射信号的物理属性值的矢量值; 根据反射系数 以及入射信号和反射信号的物理属性值的矢量值得到矢量模型的中的常数值;又例如, 根据测量得到的入射信号和反射信号的功率值获取到反射系数的幅度, 根据测量得到 的入射信号和反射信号的相位值得到反射系数的相位值; 根据多组反射系数的矢量值 以及入射信号和反射信号的物理属性值的矢量值得到矢量模型的中的常数值。 上述两 种获取方式可以单独适用也可以相互结合共同获取矢量模型中的常数值。 下面结合优选实施例进行说明, 该优选实施例结合了上述实施例及其优选实施方 式, 在本优选实施例中, 通过一种驻波比矢量检测方法消除驻波比标量检测方法通过 将驻波比检测装置抽象成一个矢量模型, 该矢量模型根据驻波比检测装置的部件及其 端口可以抽象成不同的矢量模型, 例如, 可以是双端口矢量模型, 三端口矢量模型等 等, 从而消除对驻波比检测系统的条件限制, 从而提高了驻波比的检测精度。 下面以 无线系统中驻波比双端口检测装置为例, 对本发明优选实施例的驻波比矢量检测装置 进行说明。 图 4是根据相关技术的无线系统中驻波比检测装置的示意图, 如图 4所示, 该装 置包括信号源发生器(也称为信号源产生器) 400、信号发射链路 402、信号放大器 404、 耦合器 406、 滤波器 408、 天线系统 (ANT) 410、 2选 1开关 412、 信号检测链路 414 和信号检测器 416。 下面对该装置的各个部件及其功能进行说明。 信号源发生器 400主要是产生需要发射的信号源, 需要说明的是, 其可以来自其 它设备,也可以是一个单独的信号产生器。信号发射链路 402连接至信号源发生器 400, 主要设置为完成将需要发射的信号传输出去,其可以有很多元素构成。信号放大器 404 连接至信号发射链路 402, 主要设置为完成信号的放大处理。 耦合器 406连接至信号 放大器 404, 主要设置为耦合出发射信号和反射信号, 便于进行检测。 滤波器 408连 接至耦合器 406, 主要设置为完成信号的滤波, 保证信号的发射纯度, 也可以设置为 进行收发的分离。 ANT410主要设置为发射信号。 2选 1开关 412连接至耦合器 406 和滤波器 408, 主要设置为完成发射信号和反射信号的 2选 1功能。信号检测链路 414 连接至 2选 1开关 412, 主要设置为完成发射信号和反射信号的接收, 便于进行检测, 它可以由许多独立的元素组成。 信号检测器 416连接至信号检测链路 414, 主要设置 为完成信号的检测,可以是任何具有自动处理的能力的器件(例如,常用的 CPU, DSP 和 FPGA等)。 将图 4中无线系统中驻波比检测装置为一个矢量模型,由于该装置为双端口网络, 因此, 无论入射信号和反射信号经过多少个部件传输且每个部件都是双端口, 最终抽 象为一个双端口的 S参数模型来表示。 5是根据本发明有限实施例的无线系统中驻波 比检测装置的抽象矢量模型示意图, 如图 5所示, 对该双端口的矢量模型进行说明。 如图 5所示, V™D为发射信号, V« ^为反射信号, Sll、 S12、 S21、 S22均为该 模型的参数, 根据该矢量模型可以准确的得到反射系数 的表达式为: υ,· (3) Both the incident signal and the reflected signal must be undisturbed by any other signal in the detection link during the detection process. Only when all the above three constraints are satisfied at the same time, the standing wave ratio detected by the standing wave ratio scalar detection method can be correct, and high precision can be obtained. However, it is difficult to ensure that the above three points are completely satisfied in the actual detection system (detection device). For example, the detection of the standing wave ratio in the Radio Remote Uint (RRU) in the wireless communication system, FIG. 1 is a schematic diagram of the standing wave ratio detection in the RRU in the wireless communication according to the related art, below The detection of the standing wave ratio will be described with reference to FIG. As shown in FIG. 1, the signal 1 is a transmission signal (Forward, referred to as FWD, also becomes an incident signal), and the signal 5 is a reflection signal (Reverse, abbreviated as REV). First, in the detection of the standing wave ratio, the point at which the standing wave ratio reaction is desired is the RRU and the antenna system ANT. However, after the detection point of the incident signal is placed after the component power amplifier, the power detection point of the reflected signal is placed before the component filter, so the first rule of the above limitation condition cannot be satisfied; secondly, FWD and REV are selected in 2 Before the switch passes a completely different path, it can not meet the second condition of the above limitation; Third, the detection of REV is also affected by the crosstalk signal 2 of the transmitted signal FWD, the internal signal of the system 3, the reflected interference signal of the Filter 4 Interference, therefore, cannot satisfy the third clause of the above restrictions. Based on the above analysis, the existing scalar detection method results in low accuracy of standing wave ratio detection. In practical applications, it is difficult to obtain a detection value of a higher precision standing wave ratio. SUMMARY OF THE INVENTION The present invention provides a method and apparatus for acquiring a standing wave ratio, which at least solves the problem of low accuracy and inaccuracy of standing wave ratio detection of the above-described conventional scalar standing wave ratio detecting method. According to an aspect of the present invention, a method for acquiring a standing wave ratio is provided, the method comprising: respectively acquiring a vector representation of physical property values of an incident signal and a reflected signal; and abstracting the standing wave ratio detecting device into a vector model, The parameter value of the physical expression corresponding to the vector model includes a physical attribute value of the incident signal represented by a vector and a physical attribute value of the reflected signal, and the value of the expression corresponding to the vector model is a reflection coefficient, wherein The reflection coefficient is a vector value; and the standing wave ratio is obtained according to the reflection coefficient. Preferably, obtaining a vector representation of the physical property values of the incident signal and the reflected signal respectively comprises: obtaining a vector representation of the physical property values of the incident signal and the reflected signal by measurement, respectively. Preferably, respectively obtaining a vector representation of the physical property values of the incident signal and the reflected signal comprises: respectively obtaining two different types of scalar values of the incident signal and the reflected signal by measurement, according to the different types of scalar values Obtaining a vector representation of physical property values of the incident signal and the reflected signal. Preferably, the two different types of scalar values are power values and phase values. Preferably, obtaining the constant value in the vector model comprises: acquiring a vector value of the physical property value of the fixed incident signal and the reflected signal respectively corresponding to the plurality of sets of known fixed loads obtained by using the standing wave ratio detecting device; For example, the standing wave ratio detecting means respectively corresponds to a vector value of a physical value of a fixed incident signal and a reflected signal in the case of an open circuit, a short circuit and a perfect match; and according to the reflection coefficient and the incident signal and the reflection The vector value of the physical property value of the signal results in a constant value in the vector model. Preferably, obtaining the constant value in the vector model comprises: obtaining an amplitude of the reflection coefficient according to the measured power value of the incident signal and the reflected signal, and the incident signal and the reflected signal according to the measurement The phase value obtains a phase value of the reflection coefficient; and a constant value in the vector model is obtained according to a vector value of the plurality of sets of the reflection coefficient and a vector value of the incident signal and a physical property value of the reflected signal. According to another aspect of the present invention, a standing wave ratio obtaining apparatus is further provided, the apparatus comprising: a first acquiring module configured to respectively acquire a vector representation of physical property values of an incident signal and a reflected signal; an abstract module, setting In order to abstract the standing wave ratio detecting device into a vector model, the parameter values of the physical expression corresponding to the vector model include a physical attribute value of the incident signal represented by a vector and a physical attribute value of the reflected signal, The value of the expression corresponding to the vector model is a reflection coefficient, wherein the reflection coefficient is a vector value; and the second acquisition module is configured to acquire the standing wave ratio according to the reflection coefficient. Preferably, the first acquiring module is configured to acquire the vector representation by at least one of: obtaining a vector representation of physical property values of the incident signal and the reflected signal by measurement; respectively, obtaining the incident by measurement Two different types of scalar values of the signal and the reflected signal, a vector representation of the physical property values of the incident signal and the reflected signal is obtained from the different types of scalar values. Preferably, the two different types of scalar values are power values and phase values. Preferably, the abstraction module is configured to acquire a constant value in the vector model according to at least one of the following: obtaining the transmission parameter respectively corresponding to a fixed set of fixed fixed loads obtained by using the standing wave ratio detecting device a vector value of a physical property value of the signal and the reflected signal, for example, the standing wave ratio detecting means respectively corresponds to a vector value of a physical value of the fixed incident signal and the reflected signal in the case of an open circuit, a short circuit, and a perfect match; a reflection coefficient and a vector value of a physical property value of the incident signal and the reflected signal to obtain a constant value in the vector model; acquiring the power value according to the measured incident signal and the reflected signal a magnitude of the reflection coefficient, the phase value of the reflection coefficient is obtained according to the measured phase value of the incident signal and the reflected signal; and the vector value of the plurality of sets of the reflection coefficient and the incident signal and the reflected signal The vector value of the physical property value yields a constant value in the vector model. According to the present invention, the vector detection method is adopted, and the standing wave ratio detecting device is abstracted into a vector model without using the condition limitation, and the reflection coefficient is obtained by using the expression corresponding to the vector model, and the standing wave is obtained. Therefore, the conditional limitation of the standing wave ratio scalar detection method to the standing wave ratio detection system is eliminated, and the problem of low standing wave ratio detection accuracy of the existing scalar standing wave ratio detection method is solved, and the problem of inaccuracy is effectively improved, and the station is effectively improved. The detection accuracy of the wave ratio. BRIEF DESCRIPTION OF THE DRAWINGS The accompanying drawings, which are set to illustrate,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, In the drawings: FIG. 1 is a schematic diagram of standing wave ratio detection in an RRU in wireless communication according to the related art; FIG. 2 is a flowchart of a standing wave ratio acquisition method according to an embodiment of the present invention; FIG. A block diagram of a configuration of a standing wave ratio acquisition device; 4 is a schematic diagram of a standing wave ratio detecting device in a wireless system according to the related art; FIG. 5 is a schematic diagram of an abstract vector model of a standing wave ratio detecting device in a wireless system according to a limited embodiment of the present invention; FIG. 6 is a preferred embodiment according to the present invention. FIG. 7 is a flowchart of a method for acquiring a loop delay according to a preferred embodiment of the present invention; FIG. 8 is a reflection coefficient 1 ^ according to a preferred embodiment of the present invention; FIG. 9 is a flowchart of a method for acquiring the amplitude of a channel independent reflection coefficient according to a preferred embodiment of the present invention; and FIG. 10 is a reflection coefficient of channel multiplexing according to a preferred embodiment of the present invention. A flow chart of the method of obtaining the magnitude of ^. BEST MODE FOR CARRYING OUT THE INVENTION Hereinafter, the present invention will be described in detail with reference to the accompanying drawings. It should be noted that the embodiments in the present application and the features in the embodiments may be combined with each other without conflict. In the prior art, for systems requiring VSWR detection (for example, wireless communication systems), the standing wave ratio scalar detection method is used to detect the standing wave ratio, but the use of the standing wave ratio scalar detection method is used. At least three assumptions are required to be used, but in the actual application environment, it is difficult to satisfy the three assumptions at the same time, and thus the obtained standing wave ratio is low in accuracy and inaccurate. In this embodiment, a VSWR acquisition method is provided, which is suitable for various fields of VSWR detection (for example, wireless field), and FIG. 2 is a flowchart of a VSWR acquisition method according to an embodiment of the present invention. As shown in FIG. 2, the method includes the following steps: Step S202: Acquire a vector representation of physical property values of an incident signal and a reflected signal, respectively. Step S204, abstracting the standing wave ratio detecting device into a vector model, and the parameter values of the physical expression corresponding to the vector model include physical property values of the incident signal represented by the vector and physical property values of the reflected signal, and expressions corresponding to the vector model The value is the reflection coefficient, where the reflection coefficient is a vector value. Step S206, obtaining a standing wave ratio according to the reflection coefficient. Through the above steps of the embodiment, the vector detection method is adopted, and the reflection coefficient is obtained by abstracting the standing wave ratio detecting device into a vector model without using the condition limitation, and using the expression corresponding to the vector model. And the standing wave ratio is obtained, thereby eliminating the conditional limitation of the standing wave ratio scalar detecting method on the standing wave ratio detecting system, and solving the problem that the existing scalar standing wave ratio detecting method has low accuracy and inaccuracy of standing wave ratio detection, and The detection accuracy of the standing wave ratio is effectively improved. For the vector model, there are a variety of vector models in the prior art, and different vector modules can be selected according to different needs, which will be described below in conjunction with the preferred embodiments. The manner of obtaining the vector representation of the physical attribute values of the incident signal and the reflected signal may include a plurality of types, which may be selected according to actual needs. For example, in the case where the measuring device can measure the vector, the vector measuring device can be used to obtain a vector representation of the physical property values of the incident signal and the reflected signal, respectively. This way of obtaining is simple. For another example, in the case that the measuring device can only measure the scalar quantity, the scalar measuring device can be used to respectively obtain two different types of scalar values of the incident signal and the reflected signal, and then obtain according to different types of scalar values. A vector representation of the physical property values of the incident and reflected signals. The medium acquisition method can obtain a vector representation of physical property values of the incident signal and the reflected signal on the basis of the existing scalar measuring device, and is relatively common. Of course, the above two methods can be used alone or in combination with each other to obtain a vector representation of the physical property values of the incident signal and the reflected signal. Preferably, two different types of scalar values are power values and phase values. In the vector model, the corresponding expression contains constant parameters. For a vector model, there may be different numbers of constant values (for example, three), then three sets of reflection coefficients and incident signals and reflections are required. The vector value of the physical property value of the signal constitutes three ways to calculate three different constants. That is, the number of equations corresponding to the number of constants can be constructed. The method for obtaining the constant parameters in the expression can include a plurality of types, and can be selected according to actual needs. For example, a plurality of sets of known fixed loads obtained by using the standing wave ratio detecting means may respectively obtain vector values of physical property values of the fixed incident signal and the reflected signal by acquiring the reflection coefficient, for example, the standing wave ratio detecting means is open, In the case of short circuit and perfect match, respectively, corresponding to the vector values of the physical values of the fixed incident signal and the reflected signal; respectively, and then the constant values in the vector model are obtained from the reflection coefficient and the vector value of the physical property values of the incident signal and the reflected signal. . This way of obtaining through the special values corresponding to the three special cases is general. For another example, the amplitude of the reflection coefficient is obtained according to the measured power values of the incident signal and the reflected signal, and the phase value of the reflection coefficient is obtained according to the measured phase values of the incident signal and the reflected signal; and the vector values according to the plurality of sets of reflection coefficients and The vector values of the physical property values of the incident and reflected signals result in constant values in the vector model. This method is suitable when the device that measures the data can only measure the scalar. Of course, the above methods can be used alone or in combination with each other to obtain constant parameter values in the expression. In this embodiment, a standing wave ratio obtaining device is further provided, which is used to implement the above embodiments and preferred embodiments thereof, and has not been described again, and the following relates to the device. Each module is described. As used hereinafter, the term "module" may implement a combination of software and/or hardware of a predetermined function. Although the systems and methods described in the following embodiments are preferably implemented in software, hardware, or a combination of software and hardware, is also possible and contemplated. 3 is a structural block diagram of a standing wave ratio acquisition apparatus according to an embodiment of the present invention. As shown in FIG. 3, the apparatus includes a first acquisition module 30, an abstraction module 32, and a second acquisition module 34. The module and its functions are described. The first obtaining module 30 is configured to respectively obtain vector representations of physical attribute values of the incident signal and the reflected signal; the abstract module 32 is coupled to the first obtaining module 30, and the abstracting module 32 is configured to abstract the standing wave ratio detecting device into a vector The parameter value of the physical expression corresponding to the model, the physical value of the incident signal represented by the vector and the physical property value of the reflected signal, and the value of the expression corresponding to the vector model is a reflection coefficient, wherein the reflection coefficient is a vector The second acquisition module 34 is coupled to the abstraction module 32, which is arranged to acquire the standing wave ratio based on the reflection coefficient. Preferably, the first obtaining module 30 is configured to obtain a vector representation in a plurality of manners, for example, a vector representation of physical property values of the incident signal and the reflected signal respectively by measurement; and, for example, respectively, the incident signal is obtained by measurement Two different types of scalar values of the reflected signal, according to different types of scalar values to obtain a vector representation of the physical property values of the incident signal and the reflected signal, preferably, two different types of scalar values are power values And phase values. The above two acquisition methods may be applied separately or in combination with each other to obtain a vector representation. Preferably, the abstraction module 32 can obtain the constant values in the vector model in a plurality of different manners, for example, acquiring the transmission parameters in the plurality of sets of known fixed loads obtained by using the standing wave ratio detecting means respectively corresponding to the fixed incident and reflected signals. a vector value of a physical attribute value, for example, the standing wave ratio detecting means respectively corresponds to a vector value of a physical value of a fixed incident signal and a reflected signal in the case of an open circuit, a short circuit, and a perfect match; according to the reflection coefficient and the incident signal and the reflection The vector value of the physical property value of the signal is obtained as a constant value in the vector model; for example, the amplitude of the reflection coefficient is obtained according to the measured power value of the incident signal and the reflected signal, and the phase of the incident signal and the reflected signal are obtained according to the measurement. The value obtains the phase value of the reflection coefficient; the vector value according to the plurality of sets of reflection coefficients And the vector values of the physical property values of the incident signal and the reflected signal are obtained as constant values in the vector model. The above two acquisition methods may be applied separately or in combination with each other to obtain a constant value in the vector model. The following is a description of a preferred embodiment in combination with the above-described embodiments and preferred embodiments thereof. In the preferred embodiment, the standing wave ratio scalar detection method is eliminated by a standing wave ratio vector detection method. The ratio detecting device is abstracted into a vector model, which can be abstracted into different vector models according to components of the standing wave ratio detecting device and their ports, for example, may be a dual port vector model, a three-port vector model, etc., thereby eliminating the pair The condition of the standing wave ratio detection system is limited, thereby improving the detection accuracy of the standing wave ratio. Hereinafter, a standing wave ratio vector detecting device according to a preferred embodiment of the present invention will be described by taking a standing wave ratio dual port detecting device in a wireless system as an example. 4 is a schematic diagram of a standing wave ratio detecting device in a wireless system according to the related art. As shown in FIG. 4, the device includes a signal source generator (also referred to as a signal source generator) 400, a signal transmitting link 402, and a signal amplifier. 404, coupler 406, filter 408, antenna system (ANT) 410, 2-to-1 switch 412, signal detection link 414, and signal detector 416. The various components of the device and their functions are described below. The signal source generator 400 mainly generates a signal source that needs to be transmitted. It should be noted that it may be from another device or a separate signal generator. The signal transmission link 402 is coupled to the signal source generator 400 and is primarily configured to transmit signals that need to be transmitted, which may be constructed of a number of elements. Signal amplifier 404 is coupled to signal transmission link 402 and is primarily configured to perform amplification processing of the signal. Coupler 406 is coupled to signal amplifier 404 and is primarily configured to couple the transmit and reflected signals for detection. The filter 408 is connected to the coupler 406, and is mainly configured to complete the filtering of the signal to ensure the transmission purity of the signal, and may also be set to perform separation of the transmission and reception. The ANT410 is primarily set to transmit signals. The 2-to-1 switch 412 is coupled to the coupler 406 and the filter 408, and is primarily configured to perform a 2-to-1 function of the transmitted and reflected signals. The signal detection link 414 is connected to the 2-to-1 switch 412, which is primarily configured to complete the reception of the transmitted and reflected signals for easy detection. It can be composed of a number of independent elements. Signal detector 416 is coupled to signal detection link 414, primarily to detect the completion of the signal, and can be any device with automatic processing capabilities (eg, conventional CPUs, DSPs, FPGAs, etc.). The VSWR detection device in the wireless system of FIG. 4 is a vector model. Since the device is a two-port network, no matter how many components of the incident signal and the reflected signal are transmitted and each component is a dual port, the final abstraction is A dual port S-parameter model is used to represent. 5 is a schematic diagram of an abstract vector model of a standing wave ratio detecting device in a wireless system according to a limited embodiment of the present invention. As shown in FIG. 5, the vector model of the dual port will be described. As shown in FIG. 5, V TMD is a transmission signal, V « ^ is a reflection signal, and S11, S12, S21, and S22 are parameters of the model. According to the vector model, an expression of the reflection coefficient can be accurately obtained as follows: Oh,
(6), 其中,
Figure imgf000010_0001
入公式 (6) 可知: 只要可以得出在公式 (6) 中的 "^ 22' , 就可以准确的 求出反射系数 。 由于 Sll、 S12、 S21、 S22均为该模型的参数, 且上述参数均为常数,
(6), among them,
Figure imgf000010_0001
Entering the formula (6), we can see that the reflection coefficient can be accurately obtained as long as the "^ 22 ' in the formula (6) can be obtained. Since S11, S12, S21, and S22 are the parameters of the model, and the above parameters Are constant,
S22 = B, ST S 22 = B, S T
因此可以将 Λιι 22' 三个量用三个常数来代替这里用 Λ" 来代替, 其中, A, B, C 三个常量为复数具有相位和幅度特性。 根据以上的替换, 公式 (6) 可以转换为公式 (7)。 Can thus be Λ ιι 22 'by an amount of three three constants used here instead of Λ "in place, wherein, A, B, C is a constant complex number having a three phase and amplitude characteristics. According to the above alternatives, the formula (6) Can be converted to formula (7).
B * S, -A *B + C (7); 下面将根据公式 (7) 对本优选实施例的计算步骤进行如下说明, 对于公式 (7) 中的常数的求解方法可以有多种。 方法一、 通过获取反射系数在驻波比检测装置为开路、 短路和完全匹配的情况下 对应的矢量值, 其中, 开路、 短路和完全匹配分别对应固定的入射信号和反射信号的 物理属性值的矢量值; 然后, 根据反射系数以及入射信号和反射信号的物理属性值的 矢量值得到矢量模型的中的常数值。 步骤一、 可以采用方法二中的求解相位和幅度的方法来实时的计算得到。 步骤二、 三个未知数可以用1 ^为已知的三种情况来获取得到,不失一般性, 通常用三种特殊的情况即开路, 短路和匹配来联立三个方程式获取。 这三种情况对应 的 1 ^ 1分为为 0, -1和 1三个值, 相位分别对应的是 0, 180和 0。 同时在这三种情况 下可以分别计算出 ^κ^-^^ , 其中, '"-Μ '为匹配情况下的 "值, '"-°,为开路情 况下的 "值, 为短路情况下的 "值, 这样, 通过三组已知量就可以计算出公式 (7) 中的常数量 AAC。 步骤三、 通过联立方程组可以计算得到: B * S, -A *B + C (7); The calculation steps of the preferred embodiment will be described below according to the formula (7), and there are various methods for solving the constant in the formula (7). Method 1 : Obtain a reflection coefficient corresponding to a vector value in the case where the standing wave ratio detecting device is open, short, and fully matched, wherein the open circuit, the short circuit, and the perfect match respectively correspond to the physical values of the fixed incident signal and the reflected signal. Vector value; Then, a constant value in the vector model is obtained from the reflection coefficient and the vector value of the physical property values of the incident signal and the reflected signal. Step one can be calculated in real time by using the method of solving the phase and amplitude in the second method. Step 2: The three unknowns can be obtained by using 1 ^ for three known cases without loss of generality. Usually, three special cases are used, namely open circuit, short circuit and matching to obtain three equations. The 1 ^ 1 corresponding to these three cases is divided into three values of 0, -1 and 1, and the phases correspond to 0, 180 and 0, respectively. At the same time, in these three cases, ^κ^-^^ can be calculated separately, where '"- Μ ' is the value of the matching case, '"-°, which is the value of the open circuit case, in the case of short circuit The "value, so that the constant number of AACs in equation (7) can be calculated from three sets of known quantities. Step three, through the simultaneous equations can be calculated:
A = SiA = S i
e _ e C = 2(S,.„—。―e _ e C = 2(S,.„—.―
Figure imgf000011_0001
通常这三组值可以提前获取并保存 步骤四、利用公式(7 )同时结合步骤三中提前获得量就可以准确的获取反射系数
Figure imgf000011_0001
Usually these three sets of values can be obtained in advance and saved in step four. Using the formula (7) and the advance amount obtained in step three can accurately obtain the reflection coefficient.
Γ 并且, 由于所有的计算过程均是采用矢量值计算, 则得到的反射系数 也是矢 量值, 公式(7 ) 中所有的量都是矢量, 任何一个矢量都具有幅度和相位信息。 从而准 确地获取到驻波比。 方法二、 根据测量得到的入射信号和反射信号的功率值获取到反射系数的幅度, 根据测量得到的入射信号和反射信号的相位值得到反射系数的相位值; 根据多组反射 系数的矢量值以及入射信号和反射信号的物理属性值的矢量值得到矢量模型的中的常 数值。 在测量数据的装置只能测量标量的情况下, 这种方式比较适用。 当然上述方式 可以单独使用, 也可以相互结合来获得表达式中的常量参数值。 图 6是根据本发明优选实施例的抽象得到的反射信号检测路径和入射信号检测路 径的示意图, 如图 6所示, 需要说明的是, 在驻波比检测系统中无论信号传输进过了 多少个部件, 总可以抽象为一个反射信号检测路径和入射信号检测路径。 在进行幅度和相位检测之前, 首先需要获取前向信号 ΤΧ检测点到入射信号 FWD 检测点之间的环路延迟, 只有知道了环路的延迟, 那么在开始检测前向信号后在延迟 一个环路延迟的时间去检测发射信号和反射信号, 才能确保这两部分信号是同一段信 号产生, 提前获取环路的延迟后便于计算各个信号的相位和幅度。 图 7是根据本发明 优选实施例的获取环路延迟方法的流程图, 如图 7所示, 该方法包括如下步骤: 步骤 S702, 打开信号源产生器。 步骤 S704, 同时采集信号源产生的信号 ΤΧ和经过传输后的入射信号 FWD。 步骤 S706, 将 TX信号和 FWD信号做相关处理求出相关峰值。 步骤 S708 , 判断是否存在相关峰值, 在判断为是的情况下, 转至步骤 S712, 在 判断为否的情况下, 执行步骤 S710。 步骤 S710, 增加 FWD信号的采样长度, 转至步骤 S704。 步骤 S712, 获取相关峰值对应的点。 步骤 S714, 获取整个环路的延迟。 下面结合图 6所示的抽象的到的路经检测的示意图对反射系数 的相位和幅度的 计算方法及步骤进行说明。 图 8是根据本发明优选实施例的反射系数1^的相位的获取方法的流程图, 如图 8 所示, 该方法包括如下步骤: 步骤 S802, 判断信号发射器是否有信号发出, 在判断结果为否的情况下, 直接结 束, 在判断为是的情况下, 执行步骤 S804。 步骤 S804, 将射频开关选择到 FWD, 在确保开始采集信号源发出信号 TX时和 开始采集发射信号 FWD时的延迟为环路延迟情况下同时采集 TX和 FWD相同长度数 据并保存。 步骤 S806, 将射频开关选择到 REV, 在确保开始采集信号源发出信号 TX时和开 始采集反射信号 REV时的延迟为环路延迟情况下同时采集 TX和 REV相同长度数据 并保存。 步骤 S808, 利用采集到的 TX和 FWD数据计算出进行滑动相关处理, 找到相关 峰值后进行数据对齐处理后求出 FWD的相位相对于 TX的变化值。例如,在某一个时 刻如 T0, 同时采集 TXO和 FWD0的一段数据, 然后通过相关对齐处理后, 可以计算 出 FWD0相对于 TX0的相位变化量 Δφ()。 步骤 S810, 利用采集到的 TX和 REV数据计算出进行滑动相关处理, 找到相关 峰值后进行数据对齐处理后求出 REV的相位相对于 TX的变化值。 例如, 如果 FWD 和 REV的检测通道各自独立,那么在采集前向数据的同时也同时采集 TO时刻的 TX0 和 REVO的一段数据, 然后通过相关对齐处理后, 可以计算出 REVO相对于 TX0的相 位变化量ΔΨQ。 又例如, 如果 FWD和 REV检测的通道复用, 那么在完成前向采集后 间隔秒量级的时间内目的是保证了这段时间内链路没有相位波动。 如 T1 时刻, 同时 采集 TX1和 REV1的一段数据, 同样可以 REV1相对于 TX1的相位变化量 ΔΨ1。 步骤 S812, 利用 REV相对 TX的相位差值减去 FWD相对 TX的相位差值得到 Γ Also, since all calculations are calculated using vector values, the resulting reflection coefficient is also a vector value, and all quantities in equation (7) are vectors, and any vector has amplitude and phase information. Thereby the standing wave ratio is accurately obtained. Method 2, obtaining the amplitude of the reflection coefficient according to the measured power values of the incident signal and the reflected signal, and obtaining the phase value of the reflection coefficient according to the measured phase values of the incident signal and the reflected signal; and the vector values according to the plurality of sets of reflection coefficients and The vector values of the physical property values of the incident and reflected signals result in constant values in the vector model. This method is suitable when the device that measures the data can only measure the scalar. Of course, the above methods can be used alone or in combination with each other to obtain constant parameter values in the expression. 6 is a schematic diagram of an abstracted reflected signal detection path and an incident signal detection path according to a preferred embodiment of the present invention. As shown in FIG. 6, it should be noted that, in the standing wave ratio detection system, no matter how much signal transmission has passed. The components can always be abstracted into a reflected signal detection path and an incident signal detection path. Before performing amplitude and phase detection, it is first necessary to obtain the loop delay between the forward signal ΤΧ detection point and the detection point of the incident signal FWD. Only when the delay of the loop is known, the delay is started after detecting the forward signal. The delay time of the road is to detect the transmitted signal and the reflected signal to ensure that the two parts of the signal are generated by the same segment. It is convenient to calculate the phase and amplitude of each signal after acquiring the delay of the loop in advance. FIG. 7 is a flowchart of a method for acquiring a loop delay according to a preferred embodiment of the present invention. As shown in FIG. 7, the method includes the following steps: Step S702, turning on a signal source generator. Step S704, simultaneously acquiring the signal 产生 generated by the signal source and the transmitted incident signal FWD. Step S706, correlating the TX signal and the FWD signal to obtain a correlation peak. In step S708, it is determined whether or not there is a correlation peak. If the determination is yes, the process goes to step S712. If the determination is no, the process proceeds to step S710. In step S710, the sampling length of the FWD signal is increased, and the process goes to step S704. Step S712, acquiring points corresponding to the correlation peaks. Step S714, acquiring a delay of the entire loop. The calculation method and steps of the phase and amplitude of the reflection coefficient will be described below with reference to the abstract schematic diagram of the path detection shown in FIG. 6. FIG. 8 is a flowchart of a method for acquiring a phase of a reflection coefficient 1 ^ according to a preferred embodiment of the present invention. As shown in FIG. 8, the method includes the following steps: Step S802: determining whether a signal transmitter has a signal, and determining a result If it is no, it is directly terminated. If the determination is YES, step S804 is executed. In step S804, the RF switch is selected to the FWD, and the TX and FWD data of the same length are simultaneously collected and saved while ensuring the start of the acquisition of the signal source TX signal and the start of the acquisition of the transmission signal FWD. In step S806, the RF switch is selected to the REV, and the TX and REV data of the same length are simultaneously acquired and saved in the case of ensuring the start of the acquisition of the signal source TX signal and the start of the acquisition of the reflected signal REV. Step S808: Calculate the sliding correlation process by using the collected TX and FWD data, find the correlation peak, and perform data alignment processing to determine the phase change of the FWD relative to the TX. For example, at a certain time, such as T0, a piece of data of TXO and FWD0 is simultaneously acquired, and then, after the correlation alignment process, the phase change amount Δφ() of FWD0 with respect to TX0 can be calculated. Step S810, calculating, by using the collected TX and REV data, performing a sliding correlation process, and after finding the correlation peak, performing data alignment processing to obtain a change value of the phase of the REV relative to the TX. For example, if the detection channels of FWD and REV are independent, then a piece of data of TX0 and REVO at the time of TO is simultaneously acquired while acquiring the forward data, and then the phase change of REVO with respect to TX0 can be calculated by the relevant alignment process. The amount ΔΨQ . For another example, if the channels detected by the FWD and the REV are multiplexed, the purpose of ensuring that the link has no phase fluctuation during this period of time is within the time interval of the second generation after the completion of the forward acquisition. For example, at the time T1, a piece of data of TX1 and REV1 is simultaneously acquired, and the phase change amount ΔΨ1 of REV1 with respect to TX1 can also be obtained. Step S812, using the phase difference value of the REV relative to the TX minus the phase difference value of the FWD relative to the TX
REV相对于 FWD的相位差值。 S卩, ΔΦ0禾 ρ ΔΨ0、 或 ΔΦ0和 ΔΨ1的差值就是 对应 的相位。 由于入射信号和反射信号的通道分为独立和复用两种情况,在通道独立的情况下, 相关的计算入射信号和反射信号的功率计算的相关数据可以通过测量直接获得。 但是 在通道复用的情况下, 其相关过程较为复杂。 下面对通道独立和复用两种情况下的反 射系数 ^的幅度的获取方式分别进行说明。 图 9是根据本发明优选实施例的通道独立时反射系数 ^的幅度的获取方法的流程 图, 如图 9所示, 该方法包括如下步骤: 步骤 S902, 判断信号发射器是否有信号发出, 在判断结果为否的情况下, 直接结 束, 在判断为是的情况下, 执行步骤 S904。 步骤 S904, 将射频开关选择到 FWD, 在确保开始采集信号源发出信号 TX时和 开始采集发射信号 FWD时的延迟为环路延迟情况下同时采集 TX和 FWD相同长度数 据并保存。 步骤 S906, 将射频开关选择到 REV, 在确保开始采集信号源发出信号 TX时和开 始采集反射信号 REV时的延迟为环路延迟情况下同时采集 TX和 REV相同长度数据 并保存。 步骤 S908,根据上述测量的数据以及平均功率的计算公式直接计算得出入射信号 的平均功率^。和反射信号的平均功率 。。 The phase difference of REV relative to FWD. S卩, ΔΦ0 and ρ ΔΨ0, or the difference between ΔΦ0 and ΔΨ1 is the corresponding phase. Since the channels of the incident signal and the reflected signal are divided into two cases of independent and multiplexed, in the case of independent channels, the relevant data for calculating the power calculation of the incident signal and the reflected signal can be directly obtained by measurement. However, in the case of channel multiplexing, the related process is more complicated. The manners for obtaining the amplitude of the reflection coefficient ^ in the case of channel independence and multiplexing are separately described below. FIG. 9 is a flowchart of a method for acquiring the amplitude of a channel independent reflection coefficient ^ according to a preferred embodiment of the present invention. As shown in FIG. 9, the method includes the following steps: Step S902: determining whether a signal transmitter has a signal, If the result of the determination is negative, the process is directly terminated. If the determination is YES, step S904 is executed. In step S904, the RF switch is selected to the FWD, and the TX and FWD data of the same length are simultaneously acquired and saved while ensuring the start of the acquisition of the signal source TX signal and the start of the acquisition of the transmission signal FWD. In step S906, the RF switch is selected to the REV, and the TX and REV data of the same length are simultaneously acquired and saved in the case of ensuring the start of the acquisition of the signal source TX signal and the start of the acquisition of the reflected signal REV. Step S908, directly calculating the average power of the incident signal according to the measured data and the calculation formula of the average power. And the average power of the reflected signal. .
步骤 S910, 利用
Figure imgf000013_0001
就可以得到反射系数的幅度。 图 10是根据本发明优选实施例的通道复用时反射系数 的幅度的获取方法的流 程图, 如图 10所示, 该方法包括如下步骤: 步骤 S1002, 判断信号发射器是否有信号发出, 在判断结果为否的情况下, 直接 结束, 在判断为是的情况下, 执行步骤 S1004。 步骤 S1004, 将射频开关选择到 FWD, 在确保开始采集信号源发出信号 TX时和 开始采集发射信号 FWD时的延迟为环路延迟情况下同时采集 TX和 FWD相同长度数 据并保存, 利用求相位中相关对齐就可以准确的获取到前向信号 TX的检测点和发射 信号检测点的链路的延迟 。 步骤 S1006, 将射频开关选择到 REV, 在确保开始采集信号源发出信号 TX时和 开始采集反射信号 REV时的延迟为环路延迟情况下同时采集 TX和 REV相同长度数 据并保存,凡是涉及到功率检测的系统中,检测在检测前向的时刻如 TO时刻检测 TX0 的功率。 那么在延迟7 ^即在 时刻检测反射和入射信号。 步骤 S1008,利用采集到的 TX和 FWD数据计算出两个均值功率并通过 Gtx=Pwr
Step S910, utilizing
Figure imgf000013_0001
The magnitude of the reflection coefficient can be obtained. FIG. 10 is a flowchart of a method for acquiring the amplitude of a reflection coefficient during channel multiplexing according to a preferred embodiment of the present invention. As shown in FIG. 10, the method includes the following steps: Step S1002: determining whether a signal transmitter has a signal, If the result of the determination is negative, the process is directly terminated. If the determination is YES, step S1004 is executed. In step S1004, the RF switch is selected to the FWD, and the delay of the acquisition of the signal source TX and the start of the acquisition of the transmission signal FWD are simultaneously acquired as the loop delay, and the same length data of the TX and the FWD are simultaneously collected and saved. The correlation alignment can accurately obtain the delay of the link of the forward signal TX and the link of the transmission signal detection point. In step S1006, the RF switch is selected to the REV, and the delay of the start of the acquisition of the signal source TX and the start of the acquisition of the reflected signal REV is the same as the loop delay, and the same length data of the TX and the REV are simultaneously collected and saved, where the power is involved. In the detected system, it is detected that the power of TX0 is detected at the time of detecting the forward direction, such as the TO time. Then the reflection and incident signals are detected at a time delay of 7 ^. Step S1008, calculating two average powers by using the collected TX and FWD data and passing Gtx=Pwr
(FWD) -Pwr(TX)获取环路增益, 利用求相位 Δφ0时同时获取的 TX0和 FW0数据, 分别计算出该段数据的功率, 一般是均值功率, 分别为: 。和^。, 利用这两个功 率, 就可以计算出信号整个传输路径的增益即: G = PFMX> _ P 。 步骤 S1010, 利用采集到的 TX和 REV的数据计算出两个均值功率并利用上一步 计算的环路增益计算出此刻 REV对应的 FWD, 即 Pwr (FWD) =Pwi<TX)+Gtx, 利用 求相位 ΔΨ0时同时获取的 τχο和 REVO数据,分别计算出该段数据的功率,一般是均 值功率, 分别为: Pw和 5 «^。, 利用 χ。和步骤 S1008中计算出的增益, 同时考虑到 两次计算的时间很短, 整个发射信号的路径的增益不变, 所以可以计算出在此刻的反 射信号下准确的入射信号为: P励0 = PTxo + GTXO。 步骤 S1012, 利用求得的 FWD和 REV功率即可以计算出反射系数的幅度, 分别 (FWD) -Pwr(TX) acquires the loop gain. Using the TX0 and FW0 data acquired simultaneously for the phase Δφ0 , the power of the segment data is calculated, which is generally the mean power, respectively: And ^. With these two powers, the gain of the entire transmission path of the signal can be calculated: G = P FMX > _ P . Step S1010: Calculate two average powers by using the collected TX and REV data, and calculate the FWD corresponding to the REV at the moment by using the loop gain calculated in the previous step, that is, Pwr (FWD)=Pwi<TX)+Gtx. The τχο and REVO data acquired at the same time as the phase ΔΨ0, respectively calculate the power of the segment data, generally the mean power, respectively: P w and 5 «^. , use χ. And the gain calculated in step S1008, taking into account that the time of the two calculations is short, the gain of the path of the entire transmitted signal is constant, so it can be calculated that the accurate incident signal at the current reflected signal is: P excitation 0 = P Txo + G TXO . Step S1012, using the obtained FWD and REV powers, the amplitude of the reflection coefficient can be calculated, respectively
I rL |= I r L |=
计算出的^。和 ρ« ^。利用 p wdo就可以得到反射系数的幅度。 在另外一个实施例中, 还提供了一种驻波比获取软件, 该软件用于执行上述实施 例及优选实施例中描述的技术方案。 在另外一个实施例中, 还提供了一种存储介质, 该存储介质中存储有上述软件, 该存储介质包括但不限于光盘、 软盘、 硬盘、 可擦写存储器等。 显然, 本领域的技术人员应该明白, 上述的本发明的各模块或各步骤可以用通用 的计算装置来实现, 它们可以集中在单个的计算装置上, 或者分布在多个计算装置所 组成的网络上, 可选地, 它们可以用计算装置可执行的程序代码来实现, 从而可以将 它们存储在存储装置中由计算装置来执行,或者将它们分别制作成各个集成电路模块, 或者将它们中的多个模块或步骤制作成单个集成电路模块来实现。 这样, 本发明不限 制于任何特定的硬件和软件结合。 以上所述仅为本发明的优选实施例而已, 并不用于限制本发明, 对于本领域的技 术人员来说, 本发明可以有各种更改和变化。 凡在本发明的精神和原则之内, 所作的 任何修改、 等同替换、 改进等, 均应包含在本发明的保护范围之内。 Calculated ^. And ρ « ^. The amplitude of the reflection coefficient can be obtained by using p wdo . In another embodiment, a standing wave ratio acquisition software is also provided, which is used to implement the technical solutions described in the above embodiments and preferred embodiments. In another embodiment, a storage medium is also provided, the software being stored, including but not limited to an optical disk, a floppy disk, a hard disk, a rewritable memory, and the like. Obviously, those skilled in the art should understand that the above modules or steps of the present invention can be implemented by a general-purpose computing device, which can be concentrated on a single computing device or distributed over a network composed of multiple computing devices. Alternatively, they may be implemented by program code executable by the computing device so that they may be stored in the storage device by the computing device, or they may be separately fabricated into individual integrated circuit modules, or Multiple modules or steps are made into a single integrated circuit module. Thus, the invention is not limited to any specific combination of hardware and software. The above is only the preferred embodiment of the present invention, and is not intended to limit the present invention, and various modifications and changes can be made to the present invention. Any modifications, equivalent substitutions, improvements, etc. made within the spirit and scope of the present invention are intended to be included within the scope of the present invention.

Claims

权 利 要 求 书 Claim
1. 一种驻波比获取方法, 包括: A method for obtaining a standing wave ratio, comprising:
分别获取入射信号和反射信号的物理属性值的矢量表示式; 将驻波比检测装置抽象为矢量模型, 所述矢量模型对应的物理表达式的参 数值包括使用矢量表示的所述入射信号的物理属性值和所述反射信号的物理属 性值, 所述矢量模型对应的表达式的值为反射系数, 其中, 所述反射系数为矢 量值;  Obtaining, respectively, a vector representation of physical property values of the incident signal and the reflected signal; abstracting the standing wave ratio detecting device into a vector model, the parameter value of the physical expression corresponding to the vector model including the physicality of the incident signal represented by the vector An attribute value and a physical attribute value of the reflected signal, where the value of the expression corresponding to the vector model is a reflection coefficient, wherein the reflection coefficient is a vector value;
根据所述反射系数获取所述驻波比。  The standing wave ratio is obtained according to the reflection coefficient.
2. 根据权利要求 1所述的方法, 其中, 分别获取入射信号和反射信号的物理属性 值的矢量表示形式包括: 2. The method according to claim 1, wherein the vector representations of the physical property values of the incident signal and the reflected signal are respectively obtained:
分别通过测量得到所述入射信号和反射信号的物理属性值的矢量表示式。  A vector representation of the physical property values of the incident and reflected signals is obtained by measurement, respectively.
3. 根据权利要求 1或 2所述的方法, 其中, 分别获取入射信号和反射信号的物理 属性值的矢量表示形式包括: 3. The method according to claim 1 or 2, wherein the vector representations of the physical property values of the incident signal and the reflected signal are respectively obtained:
分别通过测量得到所述入射信号和反射信号的两种不同类型的标量值, 根 据所述不同类型的标量值获取到所述入射信号和所述反射信号的物理属性值的 矢量表示式。  Two different types of scalar values of the incident signal and the reflected signal are obtained by measurement, respectively, and a vector representation of the physical property values of the incident signal and the reflected signal is obtained according to the different types of scalar values.
4. 根据权利要求 3所述的方法, 其中, 所述两种不同类型的标量值为功率值和相 位值。 4. The method of claim 3, wherein the two different types of scalar values are power values and phase values.
5. 根据权利要求 1所述的方法, 其中, 获取所述矢量模型中常数值包括: 5. The method according to claim 1, wherein obtaining a constant value in the vector model comprises:
获取所述反射系数在使用所述驻波比检测装置得到的多组已知固定负载分 别对应固定的入射信号和反射信号的物理属性值的矢量值;  Acquiring a vector value of the physical property value of the fixed incident signal and the reflected signal corresponding to the plurality of sets of known fixed loads obtained by using the standing wave ratio detecting device;
根据所述反射系数以及所述入射信号和所述反射信号的物理属性值的矢量 值得到所述矢量模型的中的常数值。  A constant value in the vector model is obtained based on the reflection coefficient and a vector value of the incident signal and the physical property value of the reflected signal.
6. 根据权利要求 1或 5所述的方法, 其中, 获取所述矢量模型中常数值包括: 根据测量得到的所述入射信号和所述反射信号的功率值获取到所述反射系 数的幅度, 根据测量得到的所述入射信号和所述反射信号的相位值得到所述反 射系数的相位值; 根据多组所述反射系数的矢量值以及所述入射信号和所述反射信号的物理 属性值的矢量值得到所述矢量模型的中的常数值。 The method according to claim 1 or 5, wherein the obtaining the constant value in the vector model comprises: obtaining the amplitude of the reflection coefficient according to the measured power value of the incident signal and the reflected signal, according to Measuring the phase values of the incident signal and the reflected signal to obtain a phase value of the reflection coefficient; A constant value in the vector model is obtained based on a plurality of sets of vector values of the reflection coefficients and vector values of physical values of the incident signal and the reflected signal.
7. 一种驻波比获取装置, 包括: 7. A standing wave ratio acquisition device, comprising:
第一获取模块, 设置为分别获取入射信号和反射信号的物理属性值的矢量 表示式;  a first acquiring module, configured to respectively obtain a vector representation of physical property values of the incident signal and the reflected signal;
抽象模块, 设置为将驻波比检测装置抽象为矢量模型, 所述矢量模型所对 应的物理表达式的参数值包括使用矢量表示的所述入射信号的物理属性值和所 述反射信号的物理属性值,所述矢量模型对应的表达式的值为反射系数,其中, 所述反射系数为矢量值;  An abstraction module, configured to abstract the standing wave ratio detecting device into a vector model, wherein the parameter value of the physical expression corresponding to the vector model includes a physical property value of the incident signal represented by a vector and a physical property of the reflected signal a value, the value of the expression corresponding to the vector model is a reflection coefficient, wherein the reflection coefficient is a vector value;
第二获取模块, 设置为根据所述反射系数获取所述驻波比。  The second obtaining module is configured to acquire the standing wave ratio according to the reflection coefficient.
8. 根据权利要求 7所述的装置, 其中, 所述第一获取模块设置为通过以下至少之 一获取所述矢量表示式: 8. The apparatus according to claim 7, wherein the first obtaining module is configured to acquire the vector representation by at least one of:
分别通过测量得到所述入射信号和反射信号的物理属性值的矢量表示式; 分别通过测量得到所述入射信号和反射信号的两种不同类型的标量值, 根 据所述不同类型的标量值获取到所述入射信号和所述反射信号的物理属性值的 矢量表示式。  Obtaining a vector representation of physical property values of the incident signal and the reflected signal by measurement; respectively obtaining two different types of scalar values of the incident signal and the reflected signal by measurement, according to different types of scalar values Obtaining a vector representation of physical property values of the incident signal and the reflected signal.
9. 根据权利要求 8所述的装置, 其中, 所述两种不同类型的标量值为功率值和相 位值。 9. Apparatus according to claim 8 wherein the two different types of scalar values are power values and phase values.
10. 根据权利要求 7所述的装置, 其中, 所述抽象模块设置为根据以下至少之一获 取所述矢量模型中常数值: 10. The apparatus of claim 7, wherein the abstraction module is configured to obtain a constant value in the vector model according to at least one of:
获取所述发射参数在使用所述驻波比检测装置得到的多组已知固定负载分 别对应固定的在入射信号和反射信号的物理属性值的矢量值; 根据所述反射系 数以及所述入射信号和所述反射信号的物理属性值的矢量值得到所述矢量模型 的中的常数值;  Obtaining, by the plurality of sets of known fixed loads obtained by using the standing wave ratio detecting device, the vector values of the physical property values of the incident signal and the reflected signal respectively; according to the reflection coefficient and the incident signal And a vector value of a physical property value of the reflected signal to obtain a constant value in the vector model;
根据测量得到的所述入射信号和所述反射信号的功率值获取到所述反射系 数的幅度, 根据测量得到的所述入射信号和所述反射信号的相位值得到所述反 射系数的相位值; 根据多组所述反射系数的矢量值以及所述入射信号和所述反 射信号的物理属性值的矢量值得到所述矢量模型的中的常数值。  Obtaining an amplitude of the reflection coefficient according to the measured power value of the incident signal and the reflected signal, and obtaining a phase value of the reflection coefficient according to the measured phase values of the incident signal and the reflected signal; A constant value in the vector model is obtained based on a plurality of sets of vector values of the reflection coefficients and vector values of physical values of the incident signal and the reflected signal.
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