JPS6159266A - Apparatus for measuring frequency - Google Patents

Apparatus for measuring frequency

Info

Publication number
JPS6159266A
JPS6159266A JP18068884A JP18068884A JPS6159266A JP S6159266 A JPS6159266 A JP S6159266A JP 18068884 A JP18068884 A JP 18068884A JP 18068884 A JP18068884 A JP 18068884A JP S6159266 A JPS6159266 A JP S6159266A
Authority
JP
Japan
Prior art keywords
circuit
frequency signal
high frequency
frequency
delay
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
JP18068884A
Other languages
Japanese (ja)
Inventor
Mikio Funai
船井 幹夫
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 JP18068884A priority Critical patent/JPS6159266A/en
Publication of JPS6159266A publication Critical patent/JPS6159266A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To attain the cost reduction of the titled apparatus, by performing delay many times by one delay line. CONSTITUTION:A high frequency signal inputted at an input port 1 is inputted not only to an I/Q phase discrimination circuit 4 through a band pass filter 2 and a distribution circuit 3a but also to a delay line 5 through a switch circuit 10. Next,a circuit 10 is changed over immediately before the high frequency signal is outputted from the line 5 and the high frequency signal outputted from the line 5 is amplified by an amplifier 11 to be inputted to a distribution circuit 3b to be divided into two and one of them is inputted to the circuit 4. The other high frequency signal of the circuit 3b is again fed back to the circuit 10 and once more inputted to the circuit 5 from the circuit 10. If a time is elapsed on and after this time while the circuit 10 is held to this state, the high frequency signal revolves succeedingly in this feedback loop to obtain a wave form V'B(t). Therefore, the high frequency signal is obtained at every delay times tau, 2tau-ntau and the output signal equal to the signal passed through the delay line just having a delay time of ntau is obtained.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は、高周波信号の搬送周波数を位相弁別器を用
いて高速に測定する装置、例えば未知のレーダ電波を広
帯域の周波数に渡って傍受する場合などに使われる周波
数測定装置に関するものである。
[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to a device for rapidly measuring the carrier frequency of a high-frequency signal using a phase discriminator, for example, when intercepting unknown radar radio waves over a wide band of frequencies. This relates to frequency measurement devices used in such applications.

〔従来技術〕[Prior art]

従来、この種の装置として第1図に示すものがあった。 Conventionally, there has been a device of this type as shown in FIG.

図において、(1)は高周波信号入力端子で、例えば未
知のレーダ電波が入力される。(2)は?ll11定周
波数の帯域幅を決定するためのバンドパスフィルタ路(
4)の出力から入力高周波信号の周波数を算出する演算
回路である。(7)は演算後のコード化した周波数情報
を出力する端子である。
In the figure, (1) is a high frequency signal input terminal, into which, for example, unknown radar radio waves are input. What about (2)? ll11 Bandpass filter path for determining the constant frequency bandwidth (
This is an arithmetic circuit that calculates the frequency of the input high-frequency signal from the output of 4). (7) is a terminal for outputting coded frequency information after calculation.

次忙従来技術の動作について説明する。The operation of the conventional technique will be explained.

第1図において、入力端子rllに人力した高周波信号
はバンドパスフィルタ(2)によって周波数を測定する
帯域幅に制限され、帯域外の不要信号は除去この高周波
信号は vA(t) =  Psin mt  (p=信号振幅
)で表わされるものとする。他方、遅延線路(5)を経
由してr/Q位相弁別回路(4)へ至る信号は、遅延時
間=τに相当する位相it=ωτ(ω;2πfは入力高
周波信号の角速度)だけ位相が異なるのでVn(t) 
= p虐ω(t+τ) で表わされる。
In Fig. 1, the high frequency signal input to the input terminal rll is limited by the bandpass filter (2) to the bandwidth for measuring the frequency, and unnecessary signals outside the band are removed. p=signal amplitude). On the other hand, the signal that reaches the r/Q phase discrimination circuit (4) via the delay line (5) has a phase corresponding to the delay time = τ = ωτ (ω; 2πf is the angular velocity of the input high-frequency signal). Since it is different, Vn(t)
It is expressed as = pω(t+τ).

ここで、/Q位相弁別回路(4)の動作については、周
知の如く、入力2信号間の位相差によって出力検波ビデ
オとして2種類(I及びQ)の正弦振幅特性が得られる
ものであって、ミキサ型、乗算器型等がある。
Here, regarding the operation of the /Q phase discrimination circuit (4), as is well known, two types (I and Q) of sine amplitude characteristics can be obtained as the output detection video depending on the phase difference between the two input signals. , mixer type, multiplier type, etc.

第2図K ミキサ型の基本構成を示す。第2図において
、(21)は高周波信号入力端子、のはローカル信号入
力端子、(23)は3db90@ハイブリツド、弼は同
相パワー分配器、(ハ)はバランスドミキサ1)(ハ)
はバランスドミキサ2、物はIF1出カ端子、田はIF
’2出力端子、弼は終端抵抗である。
Figure 2 shows the basic configuration of the K mixer type. In Figure 2, (21) is the high frequency signal input terminal, (23) is the 3db90@hybrid, (2) is the in-phase power divider, (C) is the balanced mixer 1) (C)
is balanced mixer 2, object is IF1 output terminal, field is IF
'2 output terminal, the top is the terminating resistor.

従って、上記VA(t)及びVB (t)の入力高周波
信号釦対して3/Q位相弁別回路(4)の出カニ(の及
びQ(のけ以下の如く得られる。
Therefore, for the input high-frequency signal buttons of VA(t) and VB(t), the outputs of the 3/Q phase discriminator circuit (4) and Q are obtained as follows.

I(の ”K(!IIθ Q(の = K自 θ 但し、Kは検波効率(9)を含む出力ビデオの最大振幅
を表わす定数であ5、K=に−P”で表わされるもので
ある。このときθは以下の範囲内でなければならない。
I('s ``K(!IIθ Q('s = Kself θ) where K is a constant representing the maximum amplitude of the output video including the detection efficiency (9), and is expressed as 5, K = −P'' .At this time, θ must be within the following range.

0≦ σ=ωτ=2πfτ く2π 前、4記バンドパスフイルタ(2)はこのθの範曲を決
定するためのものである◇ 従って、上記し、出力ビデオは入力周波数の変化に対し
て正弦曲線となり、この関係から逆に入力周波数を演算
することができる。
0≦ σ=ωτ=2πfτ ku2π The bandpass filter (2) mentioned above is for determining the range of this θ ◇ Therefore, as mentioned above, the output video is sine with respect to changes in the input frequency. This becomes a curve, and the input frequency can be calculated conversely from this relationship.

入力搬送周波数=f=tan−凰(Q/I)/2*r周
波数演算回路(6)は、上記演算を行な5回路であシ、
出力端子(7)から周波数情報をコード化して出力する
Input carrier frequency = f = tan - 凰 (Q / I) / 2 * r The frequency calculation circuit (6) is a 5 circuit that performs the above calculation,
Frequency information is encoded and output from the output terminal (7).

以上述べた内容は基本的構成であシ、現実には1/Q位
相弁別回路の位相誤差要因等で位相量−〇は64分割(
26)程度の分解能が限度である。従って、更に確度の
高い周波数分解能を得るためには、通常、第3図に示す
ような多段化した構成にするのが一般的である。第3図
の例では、遅延線路(5a)〜(5C)の遅延時間をそ
れぞれ1倍、4倍16倍に変えた構成を3段で行ってい
る。これによ〕、1段でsgした場合と比べて16倍に
確度を高めることが可能になル、段数を増せば更に確度
向上を図ることができる。
The above description is just the basic configuration, and in reality, the phase amount -〇 is divided into 64 (
26) resolution is the limit. Therefore, in order to obtain even more accurate frequency resolution, it is common to use a multi-stage configuration as shown in FIG. In the example shown in FIG. 3, a three-stage structure is used in which the delay times of the delay lines (5a) to (5C) are changed to 1, 4, and 16 times, respectively. With this, it is possible to increase the accuracy by 16 times compared to the case where sg is performed in one stage, and the accuracy can be further improved by increasing the number of stages.

また、第6図のように多段化して構成する場合には、遅
延線路(5a)〜(5c)の遅延時間〈は製造上で工作
精度等に起因する誤差が生じるので、各段間において周
波数演算回路(61の出方を補正する必要がある。補正
回路(9)はこの機能を行う論理回路であって、各段の
出方をそれぞれ精度の高い段からII次段間補正を行い
、最終的に最っとも精度の高い遅延線路(5c)の精度
でデータを決定するための回路である。
In addition, in the case of a multi-stage configuration as shown in Figure 6, the delay time of the delay lines (5a) to (5c) will have errors due to manufacturing precision, etc., so the frequency It is necessary to correct the output of the arithmetic circuit (61).The correction circuit (9) is a logic circuit that performs this function, and performs inter-stage correction of the output of each stage from the stage with the highest accuracy. This circuit ultimately determines data with the precision of the delay line (5c), which has the highest precision.

従来の周波数測定装置は、その周波数測定精度を向上さ
せるために遅延時間の異る遅延線路を用いて、多段に構
成していたので装置の規模が大きく、且つ高コストであ
った。
Conventional frequency measuring devices have been configured in multiple stages using delay lines with different delay times in order to improve frequency measurement accuracy, resulting in large scale and high cost devices.

〔発明の概要〕[Summary of the invention]

この発明は上記のような従来の欠点を除去する為になさ
れたもので、−個の遅延線路で信号を何度も遅延させる
ことで等価的に長時開運[線路を実現し、結果的に小型
な周波数測定装置を提供することを目的としていル。
This invention was made in order to eliminate the above-mentioned drawbacks of the conventional technology. By delaying the signal many times using - delay lines, it is possible to equivalently realize a long-time operation [line]. The purpose is to provide a compact frequency measurement device.

〔発明の実施例〕[Embodiments of the invention]

以下、この発明の一実施例を図について説明する。第4
図において、α〔は入力高周波信号と遅延線路(5)を
通過した高周波信号とを切シ替えるスイッチ回路、al
は増幅器、(11は周波数演算回路(6)の出力を遅延
線路(5)の秀嘴囃書徊り遅延時間々隔で順次記憶して
ゆくシフトレジスタである。
An embodiment of the present invention will be described below with reference to the drawings. Fourth
In the figure, α[ is a switch circuit that switches between the input high-frequency signal and the high-frequency signal that has passed through the delay line (5);
is an amplifier, and (11 is a shift register that sequentially stores the output of the frequency calculation circuit (6) at intervals of the delay time of the delay line (5).

次に動作について説明する。入力端子111から入力し
た高周波信号は従来の回路と巨1様にして、一方は分配
回路(3a)から直接0/位相弁別回路(4)へ至る。
Next, the operation will be explained. The high frequency signal inputted from the input terminal 111 is made similar to the conventional circuit, and one goes directly from the distribution circuit (3a) to the 0/phase discrimination circuit (4).

・・・・・・VA(t) 分配回路(6a)出力の他方は、最初スイッチ回路α〔
が第4図のごとく遅延線路(5)と接続された状態にな
っているので従来と同様にして遅延線路(51に至る。
・・・・・・VA(t) The other output of the distribution circuit (6a) is initially connected to the switch circuit α [
Since it is connected to the delay line (5) as shown in FIG. 4, it is connected to the delay line (51) in the same way as in the conventional case.

次に、時間がτだけ経過する直前、即ち遅Iga路(5
)から高周波信号が出力される直前にスイッチ回路0ω
を図と反対の端子に切り替える。そして、遅延線路(5
)から出力された高周波信号は増幅器Uυで増幅された
後、分配回路(3b)に至シ、信号は工 2分されて一方は従来の装置と同様に4位相弁別回路(
4)に入る。・・・・・・・・・ Vf+ (t)他方
、分配回路(6b)のもう一方の高周波信号は再びスイ
ッチ回路αOに帰環され、第4図と反対の端子に切り替
えられているスイッチ回路α0からもう7度遅延回路(
5)に入る。そして、この時間以降スイッチ回路りυが
この状態のままで時間が経過すれば、高周波信号はこの
RfJkループ内をまわル続けて第5図に示すようなy
6 (t>波形が得られる。
Next, just before the time τ has elapsed, that is, the slow Iga path (5
) Just before the high frequency signal is output from the switch circuit 0ω
Switch to the opposite terminal as shown. And the delay line (5
) is amplified by the amplifier Uυ and then sent to the distribution circuit (3b), where the signal is divided into two parts, one of which is sent to the four-phase discrimination circuit (similar to the conventional device).
4) Enter.・・・・・・・・・ Vf+ (t) On the other hand, the other high frequency signal of the distribution circuit (6b) is returned to the switch circuit αO again, and the switch circuit is switched to the opposite terminal as shown in FIG. Another 7 degrees delay circuit from α0 (
Enter 5). After this time, if the switch circuit υ remains in this state and time passes, the high frequency signal continues to circulate in this RfJk loop and becomes y as shown in Figure 5.
6 (t> waveform is obtained.

従って、遅延時間τI2τ+3’r・・・・・・・・・
・・・、nτ、・・・・・・毎に高周波信号が得られて
、あたかもnでの遅延時間をもつ遅延線路を辿った信号
と同等の出力信号として得られることになる。
Therefore, the delay time τI2τ+3'r...
A high frequency signal is obtained every time . . . , nτ, .

そして、高周波信′号v (t)及びv’B(t)は、
時々刻々−位相弁別回路(4)で位相検波され、周波数
演算回路(6)で周波数コードとじて算出される0更に
、この出力信号は、時間=τ毎にシフトレジスタ11z
に遂次読み込まれて記憶される。そして、n1時間経過
後にシフトレジスタ(LS5の記憶している周波数コー
ドは1時間毎の周波数情報で満杯となり、この情報を補
正回路(9)で従来の装置と同様に補正を行って出力端
子(7)から周波数コードとして出力すれば従来の多段
化した装置とlitじ結果を得ることができる。
Then, the high frequency signals v(t) and v'B(t) are
The phase is detected by the phase discrimination circuit (4) every moment, and the frequency code is calculated by the frequency calculation circuit (6).
are sequentially read and stored. Then, after n1 hours have elapsed, the frequency code stored in the shift register (LS5) becomes full with hourly frequency information, and this information is corrected in the correction circuit (9) in the same way as in conventional devices, and the output terminal ( 7), it is possible to obtain the same result as a conventional multi-stage device by outputting it as a frequency code.

但し、高周波信号の帰環を繰り返し行うと増幅器(1υ
で発生する雑音が次第〈成長して信号対雑音比(s/N
比)が低下して周波数の測定確度が悪化するので帰環を
無制限に続けられるわけではない。
However, if the high-frequency signal returns repeatedly, the amplifier (1υ
The noise generated in
The return cycle cannot be continued indefinitely because the frequency measurement accuracy deteriorates as the ratio) decreases.

以上、これらの経過を経て一連の動作は終了し、最初の
状態にもどせば次の高周波信号に対処できるようになる
As described above, the series of operations is completed through these steps, and by returning to the initial state, it becomes possible to deal with the next high frequency signal.

〔発明′の効果〕〔Effect of the invention〕

以上のように、この発明によれば、−個の遅延線路で信
号を何度も遅延させることで等価的に長時間遅延線路を
実現したから多段化した構成にする必要がない。したが
って、装置を安価にでき、また、少ない容積で同等の性
能を得られる効果がある。
As described above, according to the present invention, a long delay line is equivalently realized by delaying a signal many times using - number of delay lines, so there is no need for a multi-stage configuration. Therefore, the device can be made inexpensive and the same performance can be obtained with a smaller volume.

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

第1図は従来の周波数測定装置を示すブロック図、第2
図はミキサ型へ位相弁別回路の基本構成を示すブロック
図、第3図は従来装置を多段で構成した場谷のブロック
図、第4図はこの発明の一実施例による周波数測定装置
を示すブロック図、第5図はこの実施例の信号忙ついて
その時間経過を示す線図である。 (Jl・・・入力端子、(2)・・・バンドパスフィル
タ、(31・・・分配回路、(4)・・・し6位相弁別
回路、(5)・・・遅延線路、(6)・・・周波数演算
回路、(7)・・・出方端子、(8)・・・5分配回路
、(9)・・・補正回路、f11川スイッチ回路、α2
・・・シフトレジスタ。 なお、図中、同一符号//′i同一、又は相蟲部分を示
す。
Figure 1 is a block diagram showing a conventional frequency measurement device, Figure 2 is a block diagram showing a conventional frequency measurement device.
The figure is a block diagram showing the basic configuration of a mixer-type phase discrimination circuit, Figure 3 is a block diagram of a conventional device configured in multiple stages, and Figure 4 is a block diagram showing a frequency measuring device according to an embodiment of the present invention. FIG. 5 is a diagram showing the elapse of time when the signal is busy in this embodiment. (Jl...input terminal, (2)...bandpass filter, (31...distribution circuit, (4)...6 phase discrimination circuit, (5)...delay line, (6) ... Frequency calculation circuit, (7) ... Output terminal, (8) ... 5 distribution circuit, (9) ... Correction circuit, f11 river switch circuit, α2
...Shift register. In the drawings, the same reference numerals //'i indicate the same or similar parts.

Claims (1)

【特許請求の範囲】[Claims] 被測定周波数で搬送される入力高周波信号をある一定時
間遅延させることによつてその信号の位相を変える遅延
線路、この遅延線路の前段にあつて、上記入力高周波信
号と上記遅延線路通過後の高周波信号とを切り替えるス
イツチ回路、このスイツチ回路と上記遅延線路を含む帰
環ループ及びこの帰環ループの高周波信号出力と上記入
力高周波信号とを位相合成して検波し振幅が等しく互い
に90°位相の異る両極性ビデオを得るI/Q位相弁別
回路を備えたことを特徴とする周波数測定装置。
A delay line that changes the phase of an input high-frequency signal carried at the frequency to be measured by delaying it for a certain period of time, and a delay line that changes the phase of the input high-frequency signal carried by the frequency to be measured by delaying the signal for a certain period of time. A return loop including the switch circuit and the delay line, and a high-frequency signal output of the return loop and the above-mentioned input high-frequency signal are phase synthesized and detected, and the amplitudes are equal and the phase difference is 90°. A frequency measurement device comprising an I/Q phase discrimination circuit for obtaining bipolar video.
JP18068884A 1984-08-31 1984-08-31 Apparatus for measuring frequency Pending JPS6159266A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18068884A JPS6159266A (en) 1984-08-31 1984-08-31 Apparatus for measuring frequency

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18068884A JPS6159266A (en) 1984-08-31 1984-08-31 Apparatus for measuring frequency

Publications (1)

Publication Number Publication Date
JPS6159266A true JPS6159266A (en) 1986-03-26

Family

ID=16087566

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18068884A Pending JPS6159266A (en) 1984-08-31 1984-08-31 Apparatus for measuring frequency

Country Status (1)

Country Link
JP (1) JPS6159266A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5068072A (en) * 1988-12-13 1991-11-26 Sumitomo Chemical Company, Limited Electrically conductive zirconia-based sintered body and process for the production thereof

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5068072A (en) * 1988-12-13 1991-11-26 Sumitomo Chemical Company, Limited Electrically conductive zirconia-based sintered body and process for the production thereof

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