JPS617482A - Azimuth display apparatus - Google Patents
Azimuth display apparatusInfo
- Publication number
- JPS617482A JPS617482A JP10715384A JP10715384A JPS617482A JP S617482 A JPS617482 A JP S617482A JP 10715384 A JP10715384 A JP 10715384A JP 10715384 A JP10715384 A JP 10715384A JP S617482 A JPS617482 A JP S617482A
- Authority
- JP
- Japan
- Prior art keywords
- amplitude
- signal
- goniometer
- phase
- memory
- 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.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S3/00—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic or electromagnetic waves, or particle emission, not having a directional significance, are being received
- G01S3/02—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic or electromagnetic waves, or particle emission, not having a directional significance, are being received using radio waves
- G01S3/14—Systems for determining direction or deviation from predetermined direction
- G01S3/58—Rotating or oscillating beam systems using continuous analysis of received signal for determining direction in the plane of rotation or oscillation or for determining deviation from a predetermined direction in such a plane
- G01S3/60—Broad-beam systems producing in the receiver a substantially sinusoidal envelope signal of the carrier wave of the beam, the phase angle of which is dependent upon the angle between the direction of the transmitter from the receiver and a reference direction from the receiver, e.g. cardioid system
- G01S3/62—Broad-beam systems producing in the receiver a substantially sinusoidal envelope signal of the carrier wave of the beam, the phase angle of which is dependent upon the angle between the direction of the transmitter from the receiver and a reference direction from the receiver, e.g. cardioid system wherein the phase angle of the signal is indicated by a cathode-ray tube
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S3/00—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic or electromagnetic waves, or particle emission, not having a directional significance, are being received
- G01S3/02—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic or electromagnetic waves, or particle emission, not having a directional significance, are being received using radio waves
- G01S3/14—Systems for determining direction or deviation from predetermined direction
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Radar Systems Or Details Thereof (AREA)
Abstract
Description
【発明の詳細な説明】 「産業上の利用分野」 この発明は船舶等に用いられる方位表示装置に関する。[Detailed description of the invention] "Industrial application field" The present invention relates to an orientation display device used in ships and the like.
「従来技術」
従来の方位表示装置はアンテナの指向方向を回転させて
、方位成分で変調された高周波の受信信号を得るだめの
高周波ゴニオメータの回転軸に低周波ゴニオメータを連
結し、この低周波ゴニオメータに低周波信号(30KH
z)を与えることによシアンテナの指向方向の回転と同
期した互に振幅が90゜の位相差を持つ二つの平衡変調
信号を作り、この二つの平衡変調信号を高周波ゴニオメ
ータから得られる受信信号のレベルに応じて振幅変調し
た信号を得るかまたは、受信信号レベルで低周波信号を
変調した信号を低周波ゴニオメータに与えて90゜の位
相差をもつ二つの平衡変調信号を得てこの振幅変調され
た二つの平衡変調信号を陰極線管表示器のY軸とY軸に
与え、プロペラ形の映像を表示させ電波の到来方向を表
示する構造を採っている。"Prior Art" A conventional orientation display device connects a low-frequency goniometer to the rotating shaft of a high-frequency goniometer that rotates the pointing direction of the antenna and obtains a high-frequency reception signal modulated by the orientation component. low frequency signal (30KH
z) to create two balanced modulation signals with a phase difference of 90° in amplitude that are synchronized with the rotation of the pointing direction of the antenna, and convert these two balanced modulation signals into a received signal obtained from a high-frequency goniometer. Amplitude modulation is performed either by obtaining a signal amplitude modulated according to the level of the received signal, or by applying a signal obtained by modulating a low frequency signal at the received signal level to a low frequency goniometer to obtain two balanced modulation signals with a phase difference of 90°. The two balanced modulation signals thus obtained are applied to the Y-axis and Y-axis of a cathode ray tube display, and a propeller-shaped image is displayed to indicate the arrival direction of the radio waves.
「発明が解決しようとする問題点」
従来の構造によると、■低周波ゴニオメータを高周波ゴ
ニオメータと同期回転するだめの機械的構造が必要であ
る。■画周波ゴニオメータと低周波ゴニオメータの箱1
気的位相の整合調整を機械的な位朧合せによって行なう
必要があり、この調整に多くの手間が掛る。■低周波ゴ
ニオメータの設置場所に制限があるんどの欠点がある。``Problems to be Solved by the Invention'' According to the conventional structure, a mechanical structure is required to rotate the low frequency goniometer in synchronization with the high frequency goniometer. ■Picture frequency goniometer and low frequency goniometer box 1
It is necessary to perform mechanical phase matching adjustment by mechanical alignment, and this adjustment requires a lot of effort. ■The drawback is that there are restrictions on where the low frequency goniometer can be installed.
「問題点を解決するだめの手段」
この発明は電子1梱路的な構成により比較的小型かつ高
周仮ゴニオメータと独立に分離して平衡変調信号を地中
できる構造とし、配置上の制限と電気的位相の整合調整
の手間とをM?Aできる方位表示装置を提供するもので
ある。``Means for Solving Problems'' This invention has a structure that is relatively small and allows a balanced modulation signal to be underground separately from a high-frequency temporary goniometer by using an electronic one-way structure, and it overcomes restrictions on placement. M? A direction display device is provided.
この発明では正弦波と余弦波の振幅データを記憶器に記
憶させ、この記憶器をアンテナの回転、つまりゴニオメ
ータの回転と同期させて読出し、正弦波と余弦仮の振幅
位相を持つ二つの平衡変調信号を得るように構成したも
のである。In this invention, the amplitude data of sine waves and cosine waves are stored in a memory device, and this memory device is read out in synchronization with the rotation of the antenna, that is, the rotation of the goniometer, and two balanced modulations having amplitude phases of sine waves and cosine waves are generated. It is configured to obtain signals.
ここで特に記憶器に記憶する振幅データをゼロ電圧を表
わすデータで区切られた振幅変w、11パルスデータと
し、この振幅変調パルスデータを読出してDA変換する
と共にこのDA変換出力を直流阻止手段に与えることに
よりこの直流阻止手段から平衡変調信号を得ることがで
きるように構成したものである。この結果この発明によ
れば構造が簡単で然も方位成分と二相平衡゛変調信号の
位相調整を電子的手段によって行々うことかでき、よっ
て設置時の調整を簡単に行なうことができる方位表示装
置を提供できる。In particular, the amplitude data to be stored in the memory is amplitude modulation w, 11 pulse data separated by data representing zero voltage, this amplitude modulation pulse data is read out and DA converted, and the DA conversion output is sent to the DC blocking means. The structure is such that a balanced modulation signal can be obtained from this direct current blocking means by applying the following signals. As a result, according to the present invention, the structure is simple, and the phase of the azimuth component and the two-phase balanced modulation signal can be adjusted by electronic means. Display devices can be provided.
「実施例」
第1図にこの発明の一実施例を示す。図中1は指向性を
持つ一対のアンテナ、2はこのアンテナ1から方位成分
を取り出す高周波ゴニオメータ、3はゴニオメータ2の
可動コイルを回転させるモータを示す。4はロータリー
エンコーダヲ示ス。"Embodiment" FIG. 1 shows an embodiment of the present invention. In the figure, reference numeral 1 indicates a pair of antennas having directivity, reference numeral 2 indicates a high-frequency goniometer that extracts the azimuth component from the antenna 1, and reference numeral 3 indicates a motor that rotates the moving coil of the goniometer 2. 4 shows the rotary encoder.
このロータリーエンコーダ4は高周波ゴニオメータ2と
一体に回転し1回転毎に1個のパルスCK+と、02°
毎に1個のパルスCK2とを出力するものとする。5は
センス決穎用アンテナ、6A、6Bはセンススイッチ、
7は受信機、8は検波器を示す。This rotary encoder 4 rotates integrally with the high frequency goniometer 2 and outputs one pulse CK+ and 02° per rotation.
It is assumed that one pulse CK2 is output for each pulse. 5 is the antenna for sense determination, 6A and 6B are the sense switches,
7 is a receiver, and 8 is a detector.
検波器8の検波は例えば負極検波とされ、その負極性の
検波出力を方位表示装置9に供給する。Detection by the detector 8 is, for example, negative polarity detection, and the negative polarity detection output is supplied to the direction display device 9.
この発明による方位表示装置9は一対の記憶器11A
、 IIBと、この記憶器11A 、 IIBにアドレ
ス信号を与えるアドレスカウンタ12と、記憶器11A
。The direction display device 9 according to the present invention includes a pair of memory devices 11A.
, IIB, this memory 11A, an address counter 12 that provides an address signal to IIB, and the memory 11A.
.
11Bから読出されたディジタルデータをDA=mする
DA変換器13A、’、 13Bと、DA変換器13A
、 13BのDA変換出力を所定のレベルに増幅する
増幅器14A。DA converters 13A, ', 13B convert digital data read from 11B to DA=m, and DA converter 13A
, an amplifier 14A that amplifies the DA conversion output of 13B to a predetermined level.
14Bと、直流阻止手段10A 、 IOBと、直流阻
止手段10A 、 ]、OBの出力信号によって励振さ
れる共振器15A 、 15Bと、共振器15A 、
15Bの出力信号がX軸入力端子とY軸入力端子に与え
られる陰極線管表示器16と、陰極線管表示器16の輝
度変調端子Gに輝度変調端子を与え電波到来方向を決定
するセンス決定回路17とによって構成される。14B, DC blocking means 10A, IOB, DC blocking means 10A, ], resonators 15A, 15B excited by the output signal of OB, resonators 15A,
A cathode ray tube display 16 to which the output signal of 15B is applied to an X-axis input terminal and a Y-axis input terminal, and a sense determination circuit 17 which applies a brightness modulation terminal to a brightness modulation terminal G of the cathode ray tube display 16 and determines the arrival direction of radio waves. It is composed of
この発明においては一対の記憶器11AとIIBに正弦
波状の振幅データと余弦波状の振幅データを持つ振幅変
調されたパルスデータを?憶した点を特徴とするもので
ある。In this invention, amplitude-modulated pulse data having sine wave-like amplitude data and cosine-wave-like amplitude data is stored in a pair of memories 11A and IIB. It is characterized by memorized points.
この一対の記憶器11Aと11Bから読出してDA変換
した信号波形を第2図A、Hに示す。第2図AとBに示
す振幅変調パルスpaとPbはその尖頭値のエンベロー
プが正弦波と余弦層状と々るように17、全体として一
周期分のデータを記憶器IA 、 IBに欅込む。振幅
変調パルスPa 、 Pbはそれぞれ一周期の中の前半
の半周期と後半の半周期で位相を逆転させる。この振幅
変調パルスpa 、 pbを直流阻止手段10A 、
IOBに与え、振幅変調パルスpaとpbに含まれる直
流分を除去することにより第2図のCとDに示すように
半周期毎に搬送波の位相が反転するいわゆる平衡変調信
号Saとsbが得られる。The signal waveforms read from this pair of memories 11A and 11B and subjected to DA conversion are shown in FIGS. 2A and 2H. The amplitude modulated pulses pa and Pb shown in Fig. 2A and B are such that the envelopes of their peak values are sine wave and cosine layered17, and the data for one cycle is stored in the memories IA and IB as a whole. . The amplitude modulation pulses Pa and Pb each have their phases reversed in the first half cycle and the second half cycle in one cycle. These amplitude modulated pulses pa, pb are passed through the DC blocking means 10A,
By removing the DC component contained in the amplitude modulation pulses pa and pb, so-called balanced modulation signals Sa and sb, in which the phase of the carrier wave is reversed every half period, are obtained as shown in C and D of Fig. 2. It will be done.
記憶器11AとIIBは例えばROMのような半道体記
憶器を用いることができる。書込データの分解能として
は例えば0.2°ずつ変化させた振幅データをゼロデー
タと共に1アドレス毎に交互に書込む。As the memories 11A and IIB, semicircular memories such as ROMs can be used, for example. As for the resolution of the write data, for example, amplitude data changed by 0.2 degrees is written alternately with zero data for each address.
まだ撮輻方向の分解能は例えば255ステツプに刊〜子
化する。However, the resolution in the radiation direction is reduced to, for example, 255 steps.
記憶器11AとIIBはアドレスカウンタ12がら計数
出力信号が与えられ、先頭アドレスから最終アドレスま
でを繰返し読出される。この読出周期は高周波ゴニオメ
ータ2の回転周期と一致するようにロータリーエンコー
ダ4から得られる0、2°毎の分解能で出力されるパル
スCK2をアドレスカウンタ12に与え、その計数出力
をアドレス信号として記憶器11A 、”11’Bに与
えると共にゴニオメータ2が一回転する毎に発生するパ
ルスCK+にょってアドレスカウンタ12をリセットし
、ゴニオメータ2の回転と記憶器11A 、 IIBの
読出周期の関係が常に一致するようにしでいる。18は
同期回路を示しこの同期回路18によってカウンタ12
のリセットのタイミングとゴニオメータ2の基準点通過
時のタイミングを合致させるようにしている。The memories 11A and IIB are supplied with count output signals from the address counter 12, and are repeatedly read from the first address to the last address. The pulse CK2 output from the rotary encoder 4 with a resolution of 0 and 2 degrees is given to the address counter 12 so that this readout period coincides with the rotation period of the high-frequency goniometer 2, and the count output is stored as an address signal in the memory. 11A and 11'B, and the address counter 12 is reset by the pulse CK+ generated every time the goniometer 2 rotates, so that the relationship between the rotation of the goniometer 2 and the read cycle of the memories 11A and IIB always matches. Reference numeral 18 indicates a synchronous circuit, and the counter 12 is controlled by this synchronous circuit 18.
The reset timing of the goniometer 2 and the timing when the goniometer 2 passes the reference point are made to match.
ここでロータリーエンコーダ4と同期回路18トの間に
位相調整手段21を設けている。この位相調整手段21
は例えばプリセットカウンタ21Aと、このプリセット
カウンタ21Aに設定値を与える位相設定器21Bとに
よって構成することができる。位相設定器21Bは例え
ばディジタルスイッチによって構成することができる。Here, a phase adjustment means 21 is provided between the rotary encoder 4 and the synchronous circuit 18. This phase adjustment means 21
For example, it can be configured by a preset counter 21A and a phase setter 21B that provides a set value to the preset counter 21A. The phase setter 21B can be configured by, for example, a digital switch.
プリセットカウンタ21Aはアップカウンタ又はダウン
カウンタの何れを使うことができる。例えはダウンカウ
ンタを用いた場合について説明する。The preset counter 21A can be either an up counter or a down counter. For example, a case will be explained in which a down counter is used.
位相設定器21Bに遅延角度に対応する数値を設定し、
その設定した数値を同期パルスC’に+でプリセットカ
ウンタ21Aにプリセットし、そのプリセットされた数
値をパルスCK2でダウンカウントすればよい。例えば
同期パルスCK+を1°遅延させるには110.2 =
5、つまり位相設定器21Bに10進数で[5」に相
当するディジタル値を設定し、この設定値を同期パルス
CK+のタイミングでプリセットカウンタ21Aにプリ
セットし、そのプリセット値を・パルスCK2でダウン
カウントすることによりパルスCK2が5個入力される
とプリセットカウンタ21Aから桁下は信号CRiが得
られる。Set a value corresponding to the delay angle in the phase setter 21B,
The set numerical value may be preset in the preset counter 21A by adding + to the synchronizing pulse C', and the preset numerical value may be down-counted by the pulse CK2. For example, to delay the synchronization pulse CK+ by 1°, 110.2 =
5, that is, set a digital value equivalent to 5 in decimal in the phase setter 21B, preset this set value in the preset counter 21A at the timing of the synchronization pulse CK+, and count down the preset value with the pulse CK2. As a result, when five pulses CK2 are input, the signal CRi is obtained from the preset counter 21A.
従ってこの桁下げ信号CK’+を同期回路J8を通じて
アドレスカウンタ12のリセット端子Rに一体えること
により、アンテナ]の回転位相に対し記憶器11A 、
IIBの読出開始点の位相を1°分だけ遅延させるこ
とができる。よって位相設定器21Bに任意の数値を設
定することにょシ方位成分の位相と記憶器11A 、
’IIBから発生する二相平衡変調信号の位相を任意の
関係に調整することができる。この結果アンテナ1から
得られる方位成分が受信機7゜検波器8等で遅延された
としても方位成分の基進点吉二相平衡変調信号の位相を
電子的に調整することができる構造となっている。Therefore, by supplying this carry down signal CK'+ to the reset terminal R of the address counter 12 through the synchronization circuit J8, the memory 11A,
The phase of the IIB readout start point can be delayed by 1°. Therefore, by setting an arbitrary value in the phase setter 21B, the phase of the azimuth component and the memory 11A,
The phase of the two-phase balanced modulation signal generated from 'IIB can be adjusted to an arbitrary relationship. As a result, even if the azimuth component obtained from the antenna 1 is delayed by the receiver 7, the detector 8, etc., the structure allows electronic adjustment of the phase of the base point two-phase balanced modulation signal of the azimuth component. ing.
記憶器11A 、 IIBから読出された正弦振幅デー
タを持つ振幅変調パルスデータと余弦振幅データを持つ
振幅変調パルスデータはDA変換器13A 、 13B
に与えられDA変換する。このDA変換により第2図A
とBに示す振幅変調パルスpaとPbが得られる。Amplitude modulated pulse data having sine amplitude data and amplitude modulated pulse data having cosine amplitude data read from the storage devices 11A and IIB are transferred to DA converters 13A and 13B.
is given to DA conversion. By this DA conversion,
Amplitude modulated pulses pa and Pb shown in and B are obtained.
この振幅変調パルスPa 、 Pbは必要に応じて増幅
器14A 、 14Bによって所定のレベルに増幅し、
直流阻止手段ioA、 IOBに供給する。直流阻止手
段10A 、 IOBはコンデンサによって構成するこ
とができる。直流阻止手段10A 、 IOBに振幅変
調パルスpa 、 pbを与えることにょ9第2図C,
Dに示すSbのキャ゛リヤー成分の波形を正弦波状に波
形成形して陰極線管表示器16のX軸とY軸の各入力端
子に与える。These amplitude modulated pulses Pa and Pb are amplified to a predetermined level by amplifiers 14A and 14B as necessary,
Supplied to DC blocking means ioA and IOB. The direct current blocking means 10A and IOB can be constructed by capacitors. The DC blocking means 10A provides the amplitude modulation pulses pa and pb to the IOB.
The waveform of the carrier component of Sb shown in D is shaped into a sine wave and is applied to each of the X-axis and Y-axis input terminals of the cathode ray tube display 16.
一方DA変換器13A 、 13Bの基準電圧端子RE
Fに演算増幅器18から一定の直流バイアス電圧−E8
を与えると共に演算増幅器19の他方の入力端子に検波
器8の検波出力信号を与え直流バイアス電圧に検波出力
信号を重畳させ、この重畳信号をDA変換器13A 、
13Bの基準電圧端子REFに与える。On the other hand, the reference voltage terminal RE of the DA converters 13A and 13B
A constant DC bias voltage −E8 from the operational amplifier 18 to F
At the same time, the detection output signal of the wave detector 8 is applied to the other input terminal of the operational amplifier 19, and the detection output signal is superimposed on the DC bias voltage, and this superimposed signal is sent to the DA converter 13A,
13B to the reference voltage terminal REF.
17はセンス決定回路を示す。このセンス決定回路17
はセンス決定スイッチ6A 、 6Bをオンに操作する
ことによシゲート17Bを開に制御し動作状態となる。Reference numeral 17 indicates a sense determining circuit. This sense determination circuit 17
By turning on the sense decision switches 6A and 6B, the switch gate 17B is controlled to open and becomes operational.
つまシセンスアンテナ5の受信信号をゴニオメータ2で
取出した方位成分に加えると共にゲ−ト17Bを開に制
御し、このゲー) 17Bを通じて陰極線管表示器16
の輝度変調端子Gに輝度変調信号を与える。この輝度変
調信号は例えば記憶器11A 、 IIBを読出すため
のアドレス信号の最下位ビソトの信号を利用することが
できる。アドレス信号の最下位ビットの信号は平衡変調
信号Sa 、 Sbのキャリヤー成分の周波数と合致し
ており、この輝度変調信号を増幅器17C1直流阻止手
段17Dと共振器17Eを通じて陰4≠線管表示器16
の輝度変調端子G K与えることによりアンテナ1で受
信した信号成分の中の一方の極性の成分を消去し、片側
の極性のIJy分によって映出される映像だけを映出す
る。The signal received by the sense antenna 5 is added to the azimuth component extracted by the goniometer 2, and the gate 17B is controlled to open, and the cathode ray tube display 16 is passed through the gate 17B.
A brightness modulation signal is given to the brightness modulation terminal G of. As this brightness modulation signal, for example, the lowest bit signal of the address signal for reading out the memories 11A and IIB can be used. The signal of the least significant bit of the address signal matches the frequency of the carrier component of the balanced modulation signals Sa and Sb, and this brightness modulation signal is transmitted through the amplifier 17C1, the DC blocking means 17D, and the resonator 17E to the shadow 4≠ray tube display 16.
By applying the signal to the brightness modulation terminal GK, the component of one polarity among the signal components received by the antenna 1 is erased, and only the image displayed by the IJy component of one polarity is displayed.
このとき映像はプロペラ形からカージオイド形に変化し
、そのカージオイドの向によって電波の到来方向を決定
する。1.7Fはセンス決定用の輝度変調信号の極性を
設定する慣性設定回路である。この極性設定回路17F
の入力端子17AKJえる信号により輝度変調信号の極
性を選定する。この極性のス芦定は受信アンテナ1とセ
ンスアンテナ5の配置によって予め決められるものであ
り1、設置時に決められると爾後は変更されるものでな
い。At this time, the image changes from a propeller shape to a cardioid shape, and the direction of the radio wave is determined by the direction of the cardioid. 1.7F is an inertia setting circuit that sets the polarity of the brightness modulation signal for sense determination. This polarity setting circuit 17F
The polarity of the brightness modulation signal is selected by the signal sent to the input terminal 17AKJ. This polarity setting is determined in advance by the arrangement of the receiving antenna 1 and the sense antenna 5, and once it is determined at the time of installation, it cannot be changed thereafter.
「動 作」
上述したこの発明の構成によれは配憶器11Aと11B
から正弦波と余弦波の振幅変調パルスの振幅データが振
幅値ゼロのデータと共に交互に託−出されるからDA変
換器13A 、 13Bからは第2図A、Bに示すよう
に正弦波状に振幅変調された振幅変調パルスpaと余弦
波状に振幅変調された振幅変調パルスpbとを得ること
ができる。"Operation" According to the configuration of the present invention described above, the memory distributors 11A and 11B
Since the amplitude data of sine wave and cosine wave amplitude modulated pulses are sent alternately together with data of zero amplitude value, the DA converters 13A and 13B output amplitude modulation in a sine wave shape as shown in FIGS. 2A and 2B. It is possible to obtain an amplitude modulated pulse pa whose amplitude is modulated in the form of a cosine wave, and an amplitude modulated pulse pb whose amplitude is modulated in the form of a cosine wave.
受信信号が存在しない状態では演算増幅器19がらDA
変換器13A 、 13Bの各基準電圧端子REFに一
定のバイアス電圧−EBが与えられていることがら、D
A変換器13Aと13Bから出力される振幅変調パルス
pa トpbはゴニオノー220回転に同期した正弦波
及び余弦波状の振幅となる。(第3図り、Fの時点To
〜T+参照)この振幅変調パルスpaとpbを直流阻止
手段10A 、 IOBに与えることにょシ平衡変調信
号Sa(第3図E)と平衡変調信号sb(第3図G)を
得ることができる。よってこの平衡変調信号Saとsb
を共振器15A 、 15Bを通じて陰極線管表示器1
1のY軸とY軸に与えることにより陰極線管表示器11
の管面上には第4図に示すようにバイアス電圧−EI]
で決捷る半径の円が描かれる。ここで共振器15A 、
15Bを設けない場合には二相平衡変調信号Sa 、
Sbのキャリヤー信号は矩形波状のまたY軸とY軸妊
与えられることになるから、電子ビームを一方から他方
に偏向する速度が速いだめ内側が全く輝らない円が描か
れる。このような表示方法を採るときは共振器15A
、 15Bを必要としないこととなる。When there is no received signal, the operational amplifier 19
Since a constant bias voltage -EB is applied to each reference voltage terminal REF of the converters 13A and 13B, D
The amplitude modulated pulses pa to pb output from the A converters 13A and 13B have sine wave and cosine wave amplitudes synchronized with the 220 revolutions of the goniometer. (Third diagram, point F
~T+) By applying these amplitude modulated pulses pa and pb to the DC blocking means 10A and IOB, a balanced modulation signal Sa (FIG. 3E) and a balanced modulation signal sb (FIG. 3G) can be obtained. Therefore, the balanced modulation signals Sa and sb
The cathode ray tube display 1 through the resonators 15A and 15B
Cathode ray tube display 11 by giving Y-axis and Y-axis of 1
As shown in Figure 4, the bias voltage -EI] is applied on the tube surface of the
A circle with a determined radius is drawn. Here, the resonator 15A,
When 15B is not provided, two-phase balanced modulation signal Sa,
Since the Sb carrier signal has a rectangular waveform and is given a Y-axis and a Y-axis signal, the electron beam is deflected from one side to the other at a high speed, so that a circle is drawn in which the inside does not shine at all. When using such a display method, the resonator 15A
, 15B is not required.
一方例えば船舶の進路方向から90°ずれた方向から電
波が到来したとすると、検波器8の検波出力信号は第3
図Bに時点TI−T2に示すような梨形と々る。この検
波出力信号を演算と増幅器19に与えることにより演算
増幅器19の出力には第31ンICの時点T1〜T2に
示すようにバイアス電圧−E8に検波出力信号を重畳さ
せた信号が得られる。この重畳信号をDA変換器13A
、 13Bの基準電圧端子REFに与えることにより
DA変換器13A +’ 13Bからは第3図りとFの
時点TI−T2に示すような振幅に変調された振幅変q
rMパルスPa’ 、 Pb’が得られる。この振幅変
調パルスPa′、Pb′を共振器15Aと15Bに供給
することにより共振器15A 、 15Bから第3図E
とGに示す平衡f調像−qSa’とSb′が得られる。On the other hand, for example, if a radio wave arrives from a direction deviated by 90 degrees from the ship's course direction, the detected output signal of the detector 8 will be the third
Figure B shows a pear-shaped stop as shown at time TI-T2. By applying this detection output signal to the operational amplifier 19, a signal obtained by superimposing the detection output signal on the bias voltage -E8 is obtained at the output of the operational amplifier 19, as shown at times T1 to T2 of the 31st IC. This superimposed signal is transferred to the DA converter 13A.
, 13B to the reference voltage terminal REF, the DA converter 13A +' 13B outputs an amplitude modulated q modulated to the amplitude as shown at time TI-T2 in the third diagram and F.
rM pulses Pa' and Pb' are obtained. By supplying these amplitude modulated pulses Pa' and Pb' to the resonators 15A and 15B, the amplitude modulation pulses from the resonators 15A and 15B to FIG.
Equilibrium f-adjusted images -qSa' and Sb' shown in and G are obtained.
この平衡変調信号S aLとsb’を陰極線管表示器1
6のXQ’lllとY軛)に与えることによシ第5図に
示すようなプロペラ形の映像が表われる。このプロペラ
形の映像に通常行なわれているようにセンス信号を加え
てN波の到来方位を決定する。These balanced modulation signals S aL and sb' are transmitted to the cathode ray tube display 1.
6), a propeller-shaped image as shown in Fig. 5 appears. As usual, a sense signal is added to this propeller-shaped image to determine the direction of arrival of the N waves.
「効 果」
以上説明したようにこの発明によれば記憶器11AとI
IBからゼロデータで区切られた正弦波状の振幅変調パ
ルスデータと余弦波状の振幅変調パルスデータを読出し
、そのパルスデータをDA変換することによシ振幅変調
パルスpaとpbを得ると共にこの振幅変調パルスpa
とpbを曲流阻止手段10A。"Effect" As explained above, according to the present invention, the memory devices 11A and I
The amplitude modulated pulse data in the form of a sine wave and the amplitude modulated pulse data in the form of a cosine wave separated by zero data are read from the IB, and the amplitude modulated pulses pa and pb are obtained by DA converting the pulse data. pa
and pb to the bending flow prevention means 10A.
10Bに与えることにより平衡変調信号Sa 、 Sb
を得る構造としたから記憶器11A 、 IIBの読出
開始のタイミングを調整するだけでアンテナ1の回転位
相と二相平衡変調信号Sa、Sbの位相関係を調整する
ことができる。この調整は例えば位相調整手段21によ
って行なうことができ位相設定器21Bに任意の数値を
設定することによりアンテナ1の回転位相と二相平衡変
調信号Sa 、 Sbの位相を容易に調整することがで
きる。10B, the balanced modulation signals Sa, Sb
Since this structure is adopted, the rotational phase of the antenna 1 and the phase relationship between the two-phase balanced modulation signals Sa and Sb can be adjusted simply by adjusting the timing of starting reading of the memories 11A and IIB. This adjustment can be performed, for example, by the phase adjustment means 21, and by setting an arbitrary value to the phase setter 21B, the rotational phase of the antenna 1 and the phase of the two-phase balanced modulation signals Sa and Sb can be easily adjusted. .
つまり受信機7と検波器8等において方位成分信号に位
相回転を与えたとしても、その位相回転量相当分の位相
ずれを位相調整手段21によって修正することができる
。この結果設置時に要する手間は大幅に少なくできる利
点が得、られる。またアンテナ1の設置状況によ多方位
誤差が発生することがあるが、この方位誤差の修正も位
相調整手段21において行なうことができこの点でも調
整を容易に行なうことができる構造となっている。In other words, even if a phase rotation is applied to the azimuth component signal in the receiver 7, the detector 8, etc., the phase adjustment means 21 can correct a phase shift corresponding to the amount of phase rotation. As a result, there is an advantage that the effort required during installation can be significantly reduced. Furthermore, although multiple azimuth errors may occur depending on the installation condition of the antenna 1, correction of these azimuth errors can also be performed by the phase adjustment means 21, and the structure is such that adjustments can be easily made in this respect as well. .
また記憶器11A 、 IIBにゼロデータで1メ切ら
れた振幅変調パルスデータを記憶させたから、この振幅
没調パルスデータを読出してそのDA変換出力を直流阻
止手段10A 、、 IOBに与えるだけで平衡変調信
号Sa 、 Sbを得ることができるから回路構造を簡
素化することができる。In addition, since the amplitude modulation pulse data cut off by zero data is stored in the memory devices 11A and IIB, balance can be achieved simply by reading out the amplitude modulation pulse data and applying the DA conversion output to the DC blocking means 10A, IOB. Since the modulation signals Sa and Sb can be obtained, the circuit structure can be simplified.
換言すれは記憶器]、IA 、 IIBに正弦波と余弦
波の振幅データを記憶させ、この振幅データを読出して
正弦波状に振幅が変化する平衡変調信号と、余弦波状に
撮11i4が変化する平衡変調信号を得る方法が考えら
れるが、このような方法による場合は二重平衡液−器が
二つ心安となり回路構造がそれだけ複雑になる欠点があ
る。In other words, the amplitude data of sine waves and cosine waves are stored in IA and IIB, and this amplitude data is read out to generate a balanced modulation signal whose amplitude changes in the form of a sine wave, and a balanced modulation signal whose amplitude changes in the form of a cosine wave. A method of obtaining a modulation signal is conceivable, but such a method requires only two double-balanced liquid devices, which has the drawback of complicating the circuit structure.
これに対しこの発明では直流阻止手段10A、IOBに
よって平衡変調7信号に変換できるから回路構造は二重
平衡変3調器を用いる場合と比較して多いに簡素化でき
る利点が得られる。On the other hand, in the present invention, since the DC blocking means 10A and IOB can convert the signal into a balanced modulation 7 signal, the circuit structure can be greatly simplified compared to the case where a double balanced modulator is used.
「変形実施例」
上述では記憶器11A、IIBに片極性の振幅変調パル
スデータを記憶した場合を説明したが、第6図に示すよ
うにゼロを中心に正と負に振れる平衡変調信号Sa、’
Sbそのものを記憶器11A’、IIBに記憶させるこ
ともできる。この場合にはDA変換器13A、13Bか
ら直接平衡変調信号を得ることができ、直流阻止手段1
0A、IOBを必要としない。但しDA変換器13A
、 13Bは正と負のディジタル信号をDA&換するこ
とができる双極性ODA変換器を必要とする。"Modified Embodiment" In the above description, a case has been described in which unipolar amplitude modulated pulse data is stored in the memory devices 11A and IIB, but as shown in FIG. '
Sb itself can also be stored in the storage devices 11A' and IIB. In this case, a balanced modulation signal can be obtained directly from the DA converters 13A and 13B, and the direct current blocking means 1
Does not require 0A or IOB. However, DA converter 13A
, 13B requires a bipolar ODA converter that can convert positive and negative digital signals to DA&.
また他の例としては第7図に示すように例えば正極性の
直流成分EDCを持つ振幅変調パルスデータを記憶する
ように構成してもよい。この第7図の場合にはDA変換
器13A 、 13Bは片極性のディジタル信号をI)
A変換する機能のものでよい。またこの場合はDA変換
出力を直流阻止手段10A 、 IOBを介して取出す
ことによりi2図CとDに示す平衡変調信号Sa 、
Sbを得ることができる。As another example, as shown in FIG. 7, it may be configured to store amplitude modulated pulse data having, for example, a positive polarity DC component EDC. In the case of FIG. 7, the DA converters 13A and 13B convert the unipolar digital signal I)
It can be anything that has the function of converting A. Furthermore, in this case, by taking out the DA conversion output through the DC blocking means 10A and IOB, the balanced modulation signals Sa shown in Figures C and D of i2 are obtained.
Sb can be obtained.
側1図はこの発明の、一実施例を説明するだめの系統図
、第2図はこの発明の要部の動作を説明するための波形
図、第3図はこの発明による方位表示・装置全体の!1
fIJ作を説明するだめの波形図、第4図及び第5図は
万位表示装置における表示結果の例を説明するだめの1
1m1図、第6図及び第7図はこの発明の変形実施1ケ
11を説明するための波形図である。
】;受信アンテナ、2:ゴニオメータ、3:モータ、4
:1枢動回路、5:センスアンテナ、6A。
6B:センススイノチ、7:受信イ僅、8:検波器、9
:方位表示装置、]、IA 、 IIB :記憶器、1
2ニアドレスカウンタ、13A 、 13B : DA
変換器、14A 、 14B :増幅器、15A 、
15B :共撮器、16:陰極線管表示器、17:セン
ス決定回路、18二同期回路、19:演算増幅器、21
:位相調整手段、21Aニブリセツトカウンタ、21B
:位相設定器、Pa:正弦波状の振幅を持つ振幅変調パ
ルス、Pb:余弦波状の振幅を持つ振幅変調パルス、S
a:正弦波状の振幅を持つ平衡変調信号、sb:余弦波
状の振幅を持つ平衡変調信号。
特許出願人 株式会社 光電製作所代 理 人
草 野 卓手続補正書(自発)
昭和60年7月24日Figure 1 on the side is a system diagram for explaining one embodiment of this invention, Figure 2 is a waveform diagram for explaining the operation of the main parts of this invention, and Figure 3 is an overall azimuth display/device according to this invention. of! 1
Figures 4 and 5 are waveform diagrams to explain fIJ production, and Figures 4 and 5 are waveform diagrams to explain examples of display results on a ten-man display device.
1m1, FIG. 6, and FIG. 7 are waveform diagrams for explaining modified embodiment 111 of the present invention. ]; Receiving antenna, 2: Goniometer, 3: Motor, 4
:1 pivot circuit, 5: sense antenna, 6A. 6B: Sense switch, 7: Reception is weak, 8: Detector, 9
: Direction display device, ], IA, IIB : Memory device, 1
2 Near address counter, 13A, 13B: DA
Converter, 14A, 14B: Amplifier, 15A,
15B: Common camera, 16: Cathode ray tube display, 17: Sense determination circuit, 18 Two synchronization circuit, 19: Operational amplifier, 21
: Phase adjustment means, 21A nib reset counter, 21B
: Phase setter, Pa: Amplitude modulation pulse with sinusoidal amplitude, Pb: Amplitude modulation pulse with cosine wave amplitude, S
a: Balanced modulation signal with a sine wave-like amplitude; sb: Balanced modulation signal with a cosine wave-like amplitude. Patent applicant Koden Seisakusho Co., Ltd. Agent
Takashi Kusano Procedural Amendment (Voluntary) July 24, 1985
Claims (1)
転する振幅変調パルスデータを記憶した第1記憶器と、 B、余弦波状に振幅変調され半周期毎に位相が反転する
振幅変調パルスデータを記憶した第2記憶器と、 C、これら第1記憶器と第2記憶器をアンテナの指向方
向の回転と同期して読出す手段と、 D、上記第1記憶器及び第2記憶器から読出した振幅変
調パルスデータをそれぞれ振幅変調パルス信号に変換す
る一対のDA変換器と、 E、この一対のDA変換器から得られる振幅変調パルス
信号を受信信号によつて振幅変調する振幅変調手段と、 F、上記振幅変調手段から得られる平衡変調信号がX軸
及びY軸に与えられ電波の到来方向を表示す表示器と、 から成る方位表示装置。(1) A: A first memory storing amplitude modulated pulse data whose amplitude is modulated in a sine wave shape and whose phase is inverted every half cycle; B: Amplitude modulation whose amplitude is modulated in a cosine wave shape and whose phase is inverted every half cycle. a second memory storing pulse data; C. means for reading out the first memory and the second memory in synchronization with the rotation of the pointing direction of the antenna; and D. the first memory and the second memory. a pair of DA converters that convert amplitude modulated pulse data read from the device into amplitude modulated pulse signals, respectively; An azimuth display device comprising: means; F. a display device which is provided with balanced modulation signals obtained from the amplitude modulation means on the X-axis and Y-axis to display the arrival direction of radio waves.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10715384A JPS617482A (en) | 1984-05-25 | 1984-05-25 | Azimuth display apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10715384A JPS617482A (en) | 1984-05-25 | 1984-05-25 | Azimuth display apparatus |
Related Child Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP21531990A Division JPH03210490A (en) | 1990-08-15 | 1990-08-15 | Azimuth display apparatus |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS617482A true JPS617482A (en) | 1986-01-14 |
| JPH0431072B2 JPH0431072B2 (en) | 1992-05-25 |
Family
ID=14451847
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10715384A Granted JPS617482A (en) | 1984-05-25 | 1984-05-25 | Azimuth display apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS617482A (en) |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56118681A (en) * | 1980-02-25 | 1981-09-17 | Taiyo Musen Kk | Display means for direction finder |
| JPS58131574A (en) * | 1982-01-30 | 1983-08-05 | Koden Electronics Co Ltd | Direction finder |
-
1984
- 1984-05-25 JP JP10715384A patent/JPS617482A/en active Granted
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS56118681A (en) * | 1980-02-25 | 1981-09-17 | Taiyo Musen Kk | Display means for direction finder |
| JPS58131574A (en) * | 1982-01-30 | 1983-08-05 | Koden Electronics Co Ltd | Direction finder |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0431072B2 (en) | 1992-05-25 |
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