JPH04248471A - Frequency measuring device - Google Patents

Frequency measuring device

Info

Publication number
JPH04248471A
JPH04248471A JP3338291A JP3338291A JPH04248471A JP H04248471 A JPH04248471 A JP H04248471A JP 3338291 A JP3338291 A JP 3338291A JP 3338291 A JP3338291 A JP 3338291A JP H04248471 A JPH04248471 A JP H04248471A
Authority
JP
Japan
Prior art keywords
frequency
video
equalizer
circuit
amplitude
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP3338291A
Other languages
Japanese (ja)
Inventor
Yoshio Hamada
浜田 芳男
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP3338291A priority Critical patent/JPH04248471A/en
Publication of JPH04248471A publication Critical patent/JPH04248471A/en
Pending legal-status Critical Current

Links

Landscapes

  • Testing, Inspecting, Measuring Of Stereoscopic Televisions And Televisions (AREA)
  • Measuring Frequencies, Analyzing Spectra (AREA)

Abstract

PURPOSE:To enable frequency to be measured even in a wide frequency range by providing an equalizer with certain frequency characteristics at a previous stage of a phase discrimination circuit and a detection circuit of a video amplitude data which is determined by frequency characteristics at a later stage and determing frequency from the data and I/Q video quantized output. CONSTITUTION:An RF signal passed through an equalizer 10 with certain frequency characteristics and is fed to an I/Q phase discrimination circuit 5. An output QA of an adder 11 can detect a video amplitude which is determined by frequency characteristics of the equalizer 10. The video amplitude signal is converted to a quantized amplitude data, thus enabling ranges A and B of frequency measurement to be determined. A polarity is judged by a frequency calculation circuit 13 according to this amplitude data and an I/Q video, is code-converted, and is outputted as a digital data, thus enabling an uncertainty of a frequency precise measurement system of the I/Q video system to be compensated for by a rough measurement system of the amplitude data system and obtaining a high resolution.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】この発明は、パルス変調された入
力RF信号の搬送周波数を測定する周波数測定装置に関
するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a frequency measuring device for measuring the carrier frequency of a pulse-modulated input RF signal.

【0002】0002

【従来の技術】図5は例えば特開平1−152375号
公報に示された従来の周波数測定装置を簡略化したブロ
ック図である。図において、1はRF信号入力端子、2
はバンドパスフィルタ、3はRF信号を分配する分配器
、4は遅延線、5は入力信号の位相差を検出するI/Q
位相弁別回路、6はI/Qビデオを量子化するゼロクロ
ススライサ、7は周波数算出回路、8は出力端子である
。又位相弁別回路5の構成は、5aは分配器、5bは9
0°ハイブリッド、5cは検波器、5dは差動増幅器で
ある。図7は、I/Q位相弁別回路の出力ビデオ波形図
である。
2. Description of the Related Art FIG. 5 is a simplified block diagram of a conventional frequency measuring device disclosed in, for example, Japanese Patent Laid-Open No. 1-152375. In the figure, 1 is an RF signal input terminal, 2
is a bandpass filter, 3 is a distributor that distributes the RF signal, 4 is a delay line, and 5 is an I/Q that detects the phase difference of input signals.
A phase discrimination circuit, 6 a zero cross slicer for quantizing I/Q video, 7 a frequency calculation circuit, and 8 an output terminal. Further, the configuration of the phase discrimination circuit 5 is as follows: 5a is a distributor, 5b is a 9
0° hybrid, 5c is a detector, and 5d is a differential amplifier. FIG. 7 is an output video waveform diagram of the I/Q phase discrimination circuit.

【0003】次に動作について説明する。RF信号端子
1に入力したRF信号は、信号分配器3によって分配さ
れ、一方はそのままI/Q位相弁別回路5に入力され、
他方は遅延時間τを有する遅延線4を経由してI/Q位
相弁別回路5に入力される。入力された、それぞれのR
F信号は分配器5a90°ハイブリッド5bにて位相合
成されたのち、検波器5cで検波され、
Next, the operation will be explained. The RF signal input to the RF signal terminal 1 is distributed by the signal distributor 3, and one is input as is to the I/Q phase discrimination circuit 5,
The other signal is input to the I/Q phase discrimination circuit 5 via a delay line 4 having a delay time τ. Each input R
The F signal is phase-combined by a distributor 5a and a 90° hybrid 5b, and then detected by a detector 5c.

【0004】0004

【数1】[Math 1]

【数2】 但し、K=定数 θ=2πfτ(fは入力RF周波数) となることは周知の通りである。[Math 2] However, K = constant θ=2πfτ (f is input RF frequency) As is well known,

【0005】さらに上記出力V1 、V2 、V3 、
V4 は差動増幅器5dによって差動増幅されて、図6
に示すようなI/Qビデオ信号が出力してその周期は1
/τとなる。このI/Qビデオの極性をOVを基準とし
てゼロクロススライサ6で量子化し、周波数算出回路7
で極性反転した後その出力ビットをコード変換すれば、
遅延時間の逆数の1周期(1/τ)の1/4の精度で入
力周波数を算出することができる。なお、この場合はI
/Qビデオは1/τで繰り返し同じ出力となり、周波数
に対して多価となり不確定性を持つのでI/Q位相弁別
回路5の入力には測定帯域を決める、バンドパスフィル
タ2が必らず必要となる。
Furthermore, the above outputs V1, V2, V3,
V4 is differentially amplified by the differential amplifier 5d, and as shown in FIG.
The I/Q video signal shown in is output and its period is 1.
/τ. The polarity of this I/Q video is quantized by a zero cross slicer 6 using OV as a reference, and a frequency calculation circuit 7
If you reverse the polarity with and then convert the output bit,
The input frequency can be calculated with an accuracy of 1/4 of one period (1/τ) of the reciprocal of the delay time. In this case, I
/Q video has the same output repeatedly at 1/τ, has multiple values with respect to frequency, and has uncertainty. Therefore, the input of the I/Q phase discriminator circuit 5 does not necessarily include a bandpass filter 2 that determines the measurement band. It becomes necessary.

【0006】[0006]

【発明が解決しようとする課題】従来の周波数測定装置
は以上のように構成されているので、周波数測定帯域が
広くなると分解能は悪くなる、従って測定精度を保つた
めには遅延時間の異なる位相弁別回路を多段構成して周
波数分割帯域を細分し分解能を上げなければならず装置
が大規模かつ複雑となるなどの問題点があった。
[Problems to be Solved by the Invention] Conventional frequency measurement devices are configured as described above, so as the frequency measurement band becomes wider, the resolution deteriorates. Therefore, in order to maintain measurement accuracy, phase discrimination with different delay times is required. There were problems in that the circuit had to be configured in multiple stages to subdivide the frequency division band and increase the resolution, making the device large and complex.

【0007】この発明は、上記のような問題点を解消す
るためになされたものであって、測定する周波数帯域が
広くなっても精度よく周波数測定ができる安定な装置を
簡単な回路構成で得ることを目的とする。
The present invention was made to solve the above-mentioned problems, and provides a stable device with a simple circuit configuration that can measure frequencies with high accuracy even when the frequency band to be measured becomes wider. The purpose is to

【0008】[0008]

【課題を解決するための手段】この発明に係る周波数測
定装置は、I/Qビデオを出力する位相弁別回路の前段
に、一定の周波数特性を持つイコライザと、上記位相弁
別回路の右段に上記イコライザの周波数特性で決まるビ
デオ振幅データの検出回路と、そのビデオ振幅データと
I/Qビデオ量子化出力とから入力周波数を算出する周
波数算出回路とを備えたものである。
[Means for Solving the Problems] A frequency measuring device according to the present invention includes an equalizer having a certain frequency characteristic at a stage upstream of a phase discrimination circuit that outputs an I/Q video, and an equalizer having a fixed frequency characteristic at a stage to the right of the phase discrimination circuit. This device includes a video amplitude data detection circuit determined by the frequency characteristics of the equalizer, and a frequency calculation circuit that calculates an input frequency from the video amplitude data and I/Q video quantization output.

【0009】[0009]

【作用】この発明における周波数測定装置は、位相弁別
回路の前段に一定の周波数特性を持つイコライザと、位
相弁別回路の右段に上記イコライザの周波数特性で決ま
るビデオ振幅データの検出回路を設けて、そのビデオ振
幅データとI/Qビデオ量子化出力の両方から周波数を
算出するので広い周波数帯域の測定ができる。
[Operation] The frequency measuring device of the present invention includes an equalizer having a constant frequency characteristic at the front stage of the phase discrimination circuit, and a detection circuit for video amplitude data determined by the frequency characteristic of the equalizer at the right stage of the phase discrimination circuit. Since the frequency is calculated from both the video amplitude data and the I/Q video quantization output, a wide frequency band can be measured.

【0010】0010

【実施例】以下、この発明の一実施例を図について説明
する。図1は、この発明の一実施例である周波数測定装
置のブロック図であり、9はリミッテングアンプ、10
は一定の周波数特性を持たせたイコライザ、11は加算
器、12はビデオ信号を量子化するA/D変換器、13
は周波数算出回路、QA はビデオ振幅信号である。他
の符号は従来例の回路と同じである。
DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 is a block diagram of a frequency measuring device that is an embodiment of the present invention, in which 9 is a limiting amplifier, 10 is a
11 is an equalizer with constant frequency characteristics; 11 is an adder; 12 is an A/D converter that quantizes the video signal; 13
is a frequency calculation circuit, and QA is a video amplitude signal. Other symbols are the same as those in the conventional circuit.

【0011】図2ははこの発明の一実施例の動作説明図
であり、A(1/τ)はビデオ振幅データから決まる1
周期の周波数測定範囲、B(1/τ)は同じく次の1周
期の周波数測定範囲、0レベル線上の(1)−(8)は
A、Bを8等分する周波数分割帯域、a,b,c,d,
eは周波数分割帯域に対応するイコライザの周波数特性
振幅データである。
FIG. 2 is an explanatory diagram of the operation of one embodiment of the present invention, where A(1/τ) is 1 determined from video amplitude data.
The frequency measurement range of the period, B (1/τ) is the frequency measurement range of the next one period, and (1)-(8) on the 0 level line are the frequency division bands that divide A and B into 8 equal parts, a, b ,c,d,
e is frequency characteristic amplitude data of the equalizer corresponding to the frequency division band.

【0012】次に動作について説明する。RF信号入力
端子1に入力したRF信号はリミッテングアンプ9にて
出力レベルを一定にした後、一定の周波数特性を持たせ
たイコライザ10を経由してI/Q位相弁別回路5に入
力される。入力したRF信号は位相合成され検波されて
I/Qビデオが出力することは従来の動作と同じである
Next, the operation will be explained. The RF signal input to the RF signal input terminal 1 is inputted to the I/Q phase discrimination circuit 5 via the equalizer 10 having a constant frequency characteristic after the output level is made constant by the limiting amplifier 9. . The input RF signals are phase-combined and detected, and the I/Q video output is the same as in the conventional operation.

【0013】ここでイコライザ10の周波数特性が、図
2に示す様に入力周波数に対して損失特性がリニアと設
定すれば、I/Qビデオの振幅はイコライザ10の周波
数特性に従って変化する。又V3 とV4 を加算する
加算器11の出力QA は前記した数2から明らかなよ
うに入力周波数には影響されず一定のビデオ振幅となる
為に、QA としてイコライザ10の周波数特性によっ
て決められたビデオ振幅を検出できることになる。
If the frequency characteristic of the equalizer 10 is set such that the loss characteristic is linear with respect to the input frequency as shown in FIG. 2, the amplitude of the I/Q video changes in accordance with the frequency characteristic of the equalizer 10. Furthermore, the output QA of the adder 11 that adds V3 and V4 is determined by the frequency characteristics of the equalizer 10, since it is not affected by the input frequency and has a constant video amplitude, as is clear from equation 2 above. It will be possible to detect the video amplitude.

【0014】このビデオは振幅信号をA/D変換器12
によって量子化し振幅データに変換して、図2に示した
周波数測定の範囲A,Bが決定される。
This video shows how the amplitude signal is converted to the A/D converter 12.
The frequency measurement ranges A and B shown in FIG. 2 are determined by quantizing and converting into amplitude data.

【0015】この振幅データと、ゼロクロススライサ6
で量子化したI/Qビデオから周波数算出回路13で極
性判定した後コード変換して、出力端子8にディジタル
データとして出力する。
This amplitude data and the zero cross slicer 6
After determining the polarity of the I/Q video quantized by the frequency calculation circuit 13, the code is converted and outputted to the output terminal 8 as digital data.

【0016】次に周波数確定法は図2から、もともとI
/Qビデオは遅延時間の逆数の1周期1/τの1/4の
分解能があるから、1周期を4等分しイコライザ10の
周波数特性による振幅データによって決められた周波数
測定範囲A,B2周期間を■−■迄8等分とする。
Next, from FIG. 2, the frequency determination method is based on the originally I
/Q video has a resolution of 1/4 of one cycle of the reciprocal of the delay time, 1/τ, so one cycle is divided into four equal parts, and the frequency measurement range A and B determined by the amplitude data based on the frequency characteristics of the equalizer 10 are divided into two cycles. Divide the period into 8 equal parts from ■ to ■.

【0017】Aの範囲は振幅情報QA のeと対応する
■(I>0,Q>0)と、QA がdの範囲で対応する
■,■(I<0,Q<0)と、QA はcの範囲で■(
I>0,Q<0)となる。
The range of A corresponds to e of the amplitude information QA (I>0, Q>0), and the range of QA corresponds to d (I<0, Q<0), and QA is ■(
I>0, Q<0).

【0018】次にBの範囲は、QA はcの範囲で■(
I>0,Q>0)と、QA はbの範囲で■,■(I<
0,Q<0)と、QA はaの範囲で■(I>0,Q<
0)となる。
Next, the range of B is QA is the range of c, and ■(
I>0, Q>0), and QA is ■,■(I<
0, Q<0), and QA is ■(I>0, Q<0) in the range of a.
0).

【0019】イコライザ10の周波数特性で決まる振幅
データによって決定された周波数測定範囲A,BとI/
Qビデオの周波数分解能との具体的な対応関係はこの様
になり、イコライザ10は以上述べた様にその周波数特
性によって従来例の2倍の2周期間の周波数測定範囲を
決定するので従来の帯域決定のバンドパスフィルタ2は
必要ではなくなり、A,Bで従来の倍の1/8の分解能
となる。
The frequency measurement ranges A, B and I/I determined by the amplitude data determined by the frequency characteristics of the equalizer 10 are
The specific correspondence relationship with the frequency resolution of Q video is as follows. As mentioned above, the equalizer 10 determines the frequency measurement range between two periods, which is twice the conventional example, based on its frequency characteristics, so The bandpass filter 2 for determination is no longer necessary, and the resolution for A and B is 1/8 times that of the conventional method.

【0020】従ってI/Qビデオ系を周波数精測系とし
て、振幅データ系を周波数粗測系として、周波数精測系
の不確定性を周波数粗測系で補正し高分解能を得ている
Therefore, the I/Q video system is used as a frequency accurate measurement system, the amplitude data system is used as a frequency coarse measurement system, and the uncertainties of the frequency accurate measurement system are corrected by the frequency coarse measurement system to obtain high resolution.

【0021】次に周波数精測系と粗測系から周波数デー
タとして周波数算出回路13に入力する出力ビットにつ
いて述べる。I/Qビデオの8等分の周波数分割帯域を
次の様にビット表示し周波数位置データとして周波数を
確定する。 ■  A,I>0,Q>0  ■  B,I>0,Q>
0■  A,I<0,Q>0  ■  B,I<0,Q
>0■  A,I<0,Q<0  ■  A,I<0,
Q<0■  A,I>0,Q<0  ■  A,I>0
,Q<0以上の様に夫々の周波数位置をビットとして表
示して周波数算出回路13に入力しコード変換して周波
数測定が完了する。
Next, the output bits inputted to the frequency calculation circuit 13 as frequency data from the frequency precision measurement system and the coarse measurement system will be described. The frequency division band divided into eight equal parts of the I/Q video is expressed in bits as shown below, and the frequency is determined as frequency position data. ■ A, I>0, Q>0 ■ B, I>0, Q>
0 ■ A, I < 0, Q > 0 ■ B, I < 0, Q
>0 ■ A, I < 0, Q < 0 ■ A, I < 0,
Q<0 ■ A, I>0, Q<0 ■ A, I>0
, Q<0 or more, each frequency position is displayed as a bit and inputted to the frequency calculation circuit 13, where the code is converted and the frequency measurement is completed.

【0022】次にこの発明の他の実施例について図に基
づいて説明する。図3はこの発明の他の一実施例の周波
数測定回路のブロック図であり、14はI/Qビデオ周
波数算出回路であり、他の符号は前記一実施例と同じで
ある。図4はこの発明のI/Qビデオ極座標図である。 ZはI/Qビデオのベクトル、θは位相角である。
Next, another embodiment of the present invention will be explained based on the drawings. FIG. 3 is a block diagram of a frequency measurement circuit according to another embodiment of the present invention, in which 14 is an I/Q video frequency calculation circuit, and other symbols are the same as in the above embodiment. FIG. 4 is an I/Q video polar diagram of the present invention. Z is the I/Q video vector and θ is the phase angle.

【0023】次に動作について説明する。図3からRF
入力信号端子1からRF信号が入力して、位相弁別回路
5からI/Qビデオが出力する動作は前記実施例と同じ
である。
Next, the operation will be explained. From Figure 3, RF
The operation in which an RF signal is input from the input signal terminal 1 and an I/Q video is output from the phase discrimination circuit 5 is the same as in the previous embodiment.

【0024】出力したI/Qビデオを夫々A/P変換器
12で量子化して、図4の極座標におけるZ、
The output I/Q videos are each quantized by the A/P converter 12, and Z,

【数3】 を算出すれば、Zと象限から前記の実施例の図2と同様
にイコライザ10の振幅データを得ることができるので
、周波数算出回路14で周波数測定ができる。
By calculating [Equation 3], the amplitude data of the equalizer 10 can be obtained from Z and the quadrant in the same manner as in FIG.

【0025】なお上記の両実施例では、I/Q位相弁別
回路5の入力側にイコライザ10を追加して周波数特性
を持たせたものを示したが、測定帯域を決定する為のバ
ンドパスフィルタ2か又は分配器3に同様の周波数特性
を持たせても同等の効果を得ることができる。
In both of the above embodiments, an equalizer 10 is added to the input side of the I/Q phase discriminator circuit 5 to provide frequency characteristics, but a bandpass filter for determining the measurement band is used. The same effect can be obtained even if the divider 2 or the divider 3 has similar frequency characteristics.

【0026】[0026]

【発明の効果】以上の様に、この発明によればI/Qビ
デオ周波数精測系を振幅データ周波数粗測系で補正測定
する様に構成したので、簡単な回路構成で広帯域時の測
定にも分解能の高い装置が得られる効果がある。
[Effects of the Invention] As described above, according to the present invention, the I/Q video frequency precision measurement system is configured to perform corrected measurement using the amplitude data frequency coarse measurement system, so it can be used for wideband measurement with a simple circuit configuration. This also has the effect of providing a device with high resolution.

【図面の簡単な説明】[Brief explanation of the drawing]

【図1】この発明の一実施例である周波数測定装置であ
る。
FIG. 1 shows a frequency measuring device that is an embodiment of the present invention.

【図2】この発明の一実施例の動作説明図である。FIG. 2 is an explanatory diagram of the operation of an embodiment of the present invention.

【図3】この発明の他の実施例の周波数測定装置のブロ
ック図である。
FIG. 3 is a block diagram of a frequency measuring device according to another embodiment of the invention.

【図4】この発明の他の実施例の極座標図である。FIG. 4 is a polar coordinate diagram of another embodiment of the invention.

【図5】従来の周波数測定装置のブロック図である。FIG. 5 is a block diagram of a conventional frequency measurement device.

【図6】従来のI/Q位相弁別回路の出力ビデオ波形図
である。
FIG. 6 is an output video waveform diagram of a conventional I/Q phase discrimination circuit.

【符号の説明】[Explanation of symbols]

5  I/Q位相弁別回路 6  ゼロクロススライサ 7  周波数算出回路 10  イコライザ 11  加算器 12  A/D変換器 13  周波数算出回路 14  周波数算出回路 なお、図中、同一符号は同一または相当部分を示す。 5 I/Q phase discrimination circuit 6 Zero cross slicer 7 Frequency calculation circuit 10 Equalizer 11 Adder 12 A/D converter 13 Frequency calculation circuit 14 Frequency calculation circuit In addition, in the figures, the same reference numerals indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  RF信号を位相弁別してI/Qビデオ
を出力するI/Q位相弁別回路と、上記I/Qビデオ出
力を量子化するゼロクロススライサと、上記I/Q量子
化出力を周波数データに変換する周波数算出回路とを備
えた周波数測定装置において、上記位相弁別回路の前段
に設けられた一定の周波数特性を持つイコライザと、上
記位相弁別回路の後段に設けられた上記イコライザの周
波数特性で決まるビデオ振幅データの検出回路と、その
ビデオ振幅データと上記I/Qビデオ量子化出力から入
力周波数を算出する周波数算出回路とを備えたことを特
徴とする周波数測定装置。
1. An I/Q phase discrimination circuit that discriminates the phase of an RF signal and outputs an I/Q video, a zero cross slicer that quantizes the I/Q video output, and converts the I/Q quantized output into frequency data. In the frequency measuring device, the frequency measuring device is equipped with an equalizer having a certain frequency characteristic provided before the phase discrimination circuit, and a frequency characteristic of the equalizer provided after the phase discrimination circuit. 1. A frequency measurement device comprising: a detection circuit for determined video amplitude data; and a frequency calculation circuit for calculating an input frequency from the video amplitude data and the I/Q video quantized output.
JP3338291A 1991-02-04 1991-02-04 Frequency measuring device Pending JPH04248471A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3338291A JPH04248471A (en) 1991-02-04 1991-02-04 Frequency measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3338291A JPH04248471A (en) 1991-02-04 1991-02-04 Frequency measuring device

Publications (1)

Publication Number Publication Date
JPH04248471A true JPH04248471A (en) 1992-09-03

Family

ID=12385044

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3338291A Pending JPH04248471A (en) 1991-02-04 1991-02-04 Frequency measuring device

Country Status (1)

Country Link
JP (1) JPH04248471A (en)

Similar Documents

Publication Publication Date Title
JPH07154378A (en) Optical transmission characteristic measuring instrument
US4637072A (en) Method of measuring the dispersion of a transmitting optical fibre
JPH0146034B2 (en)
JPH04248471A (en) Frequency measuring device
US4685075A (en) Apparatus for measuring propagation time of ultrasonic waves
RU2225012C2 (en) Phase-meter
JPS5834372A (en) Measurement system for c/n ratio
JPS59195166A (en) Rough measuring method of frequency
EP0546851A1 (en) Digital data detector
SU1559303A1 (en) Device for measuring phase characteristics of four-terminal network
JPS6134100B2 (en)
JP2856042B2 (en) Radar equipment for vehicles
JPS594667B2 (en) Center frequency measurement method for narrowband irregular signals
SU970257A1 (en) Signal phase fluctuation measuring method
RU2027318C1 (en) Parameter measurement method for channels characterized by phase distortions
JPH0371063A (en) Frequency measuring instrument
JPH04100424A (en) Instrument and method for measuring delay time
SU1094000A1 (en) Method of determination of measuring converter static error
SU1093987A1 (en) Frequency meter
SU1061276A1 (en) Device for measuring signal reception quality in radio-communication channels
SU1103162A1 (en) Method of measuring noise of digital filter perform multi-point discrete fourier transform
JPS6324450Y2 (en)
JPH0682500A (en) Frequency measuring device
JPS5915324A (en) Measuring device for phase difference
SU1265478A1 (en) Correlation flowmeter