JPS5921104A - Digital control oscillator - Google Patents

Digital control oscillator

Info

Publication number
JPS5921104A
JPS5921104A JP57130825A JP13082582A JPS5921104A JP S5921104 A JPS5921104 A JP S5921104A JP 57130825 A JP57130825 A JP 57130825A JP 13082582 A JP13082582 A JP 13082582A JP S5921104 A JPS5921104 A JP S5921104A
Authority
JP
Japan
Prior art keywords
output
digital
adder
addition
frequency
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP57130825A
Other languages
Japanese (ja)
Inventor
Mikio Sasaki
幹雄 佐々木
Kazunori Yamate
万典 山手
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP57130825A priority Critical patent/JPS5921104A/en
Publication of JPS5921104A publication Critical patent/JPS5921104A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03KPULSE TECHNIQUE
    • H03K4/00Generating pulses having essentially a finite slope or stepped portions
    • H03K4/02Generating pulses having essentially a finite slope or stepped portions having stepped portions, e.g. staircase waveform
    • H03K4/026Generating pulses having essentially a finite slope or stepped portions having stepped portions, e.g. staircase waveform using digital techniques

Landscapes

  • Stabilization Of Oscillater, Synchronisation, Frequency Synthesizers (AREA)

Abstract

PURPOSE:To obtain an oscillating output of high accuracy, by calculating and storing a product obtained by multiplying a digital signal sampled with a prescribed sampling frequency by the 1st digital coefficient, the 2nd digital coefficient and the calculated result obtained earlier by a sampling period respectively. CONSTITUTION:A digital signal V(nT) sampled with a prescribed sampling frequency FS is supplied to an input terminal 1 and multiplied by the 1st digital coefficient C1 through a multiplier 2. A data selector 3 selects data with a selection pulse t1, and the code is checked by a decoder 6. Then the addition or subtraction is selected by an FF7. An adder 4 performs an addition with a sampling period earlier output y(nT) supplied from a D-FF5, and then C2 is selected and added. In this case, if the adder 4 has an overflow, this overflow is detected by the decoder 6. The output of addition is inverted to deliver the correct value in the form of a triangular wave. At the same time, a subtraction is carried out via the FF7. These actions are repeated to obtain an oscillating output of a triangular wave. Both oscillating frequency and control sensitivity can be controlled by changing the coefficients C1 and C2.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、ディジクル制御により所定波形の発振出力を
発生するディジクル制御形の発振器に関し、比較的簡単
な構成で発振出力を精度良く発生することのできる発振
器を提供しようとするものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a digital control type oscillator that generates an oscillation output of a predetermined waveform by digital control, and is capable of generating an oscillation output with high precision with a relatively simple configuration. The aim is to provide an oscillator.

従来例の構成とその問題点 一般に、電圧制御発振器(VCO)はアナログ回路では
PLL復調回路等で広範囲に使用さnているが、正弦波
発振器は回路構成も複雑で周波数の可変範囲や直線性に
ついても高度な技術を要するものであるところから、回
路構成の簡単な三角jツや鋸歯状波の発振器がよく使用
されている。
Conventional configurations and their problems In general, voltage-controlled oscillators (VCOs) are widely used in analog circuits such as PLL demodulation circuits, but sine wave oscillators have complex circuit configurations and problems with variable frequency range and linearity. Since this also requires advanced technology, triangular or sawtooth wave oscillators with simple circuit configurations are often used.

一方、ティジクル形の■COでも正弦波発振器としてR
OMテーブルケ利用したり、規模の大きな乗算器を用い
た2涸の1次ローバスフィルターを従続接続して帰還さ
せる、いわゆるクワドラチャタイプのvCOなどがある
が、いずn.も構成が複雑で実用的なものではない。し
かし,PLL回略で使用するvCOとしては正確な正弦
波のものでなくても高周波分が多少含まれていても動作
に大きな影響を与えない.という特性がある。.81♀
1的.・.・・.・ 本発明は、入tj信?号’2pLb復調する面路に″扇
いて最適な7”イジタル制御発振器を提供するもので、
特に、比較的簡単な構成であってしかも発振出力を精度
良く発生することのできるものを提供することを目的と
するものである。
On the other hand, even with the Tizicle type ■CO, R can be used as a sine wave oscillator.
There are so-called quadrature-type vCOs that use OM table filters, and that use two first-order low-pass filters using large-scale multipliers connected in series, but none of them. However, the configuration is complicated and not practical. However, even if the vCO used in the PLL circuit is not an exact sine wave, even if it contains some high frequency components, it will not have a major effect on the operation. There is a characteristic that .. 81♀
1 target.・..・・・.・ Is the present invention based on input information? It provides an optimal 7" digitally controlled oscillator for the surface path for demodulating 2pLb signal.
In particular, it is an object of the present invention to provide a device that has a relatively simple configuration and can generate an oscillation output with high accuracy.

発明の構成.. 本発明においては、捷ず、所定の標本化周波数F+で標
本化さfL.たディジタル信号を入力とする。
Structure of the invention. .. In the present invention, fL is sampled at a predetermined sampling frequency F+ without being switched. The input is a digital signal.

そして、その入力に第1のディジクル係数01を損け、
その積と第2のディジクル係数02と1標本化周期前の
で算結果y((..n−1)T>との3つのディジタル
信号を演算手段により演算する。
Then, add the first dicicle coefficient 01 to that input,
The calculation means calculates three digital signals: the product, the second digital coefficient 02, and the calculation result y((..n-1)T> of one sampling period before).

その演算結果.Y(nT)t−出力信号として出力する
とともに,次の標本化時の演算用として記憶するように
した点に特徴がある。
The result of the calculation. It is characterized in that it is output as a Y(nT)t-output signal and is also stored for use in calculations during the next sampling.

実施例の説明 以下、本発明の一実施例につき図面全参照して説明する
DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below with reference to all the drawings.

.1まず、第1図にPI,L復調回路の基本構成を示.
LOここでPDは位相検波器、L,PFはロー,シス?
フィシレク巨、vCOは電圧制御形の発振器である。
.. 1 First, Figure 1 shows the basic configuration of the PI,L demodulation circuit.
LO Here, PD is a phase detector, L, PF are low, cis?
Fisilek Giant and vCO are voltage controlled oscillators.

v′COは基本的に周波数変調器であり、制御信号の振
幅に比例した周波数の発振出力全発生−i4.ものであ
る。すなわち、vGOでは制御信号の電圧Vと発振出力
の角周波数Wとの間に (W7W[l),=OV なる関係がある。ここで、WOはvCOの中心周波数、
Cは定数である。発振出力の位相をψとすると、dψ/
dt==Wより、 となる。そこで、t二nT(nは整数5Tは標本化周期
辷としてψ(a?時間離散値ψ(nT)で表わせば、と
なる。ここで、ψ(nT)t引数とするコサイン変換を
行クて.Y(nT)’k求めれば、vGOの発振出力が
演算されたことになる。
v'CO is essentially a frequency modulator, which generates an oscillating output with a frequency proportional to the amplitude of the control signal -i4. It is something. That is, in vGO, there is the following relationship between the voltage V of the control signal and the angular frequency W of the oscillation output: (W7W[l),=OV. Here, WO is the center frequency of vCO,
C is a constant. If the phase of the oscillation output is ψ, then dψ/
From dt==W, it becomes. Therefore, if expressed as ψ(a? time discrete value ψ(nT)) where t2nT(n is an integer and 5T is the sampling period length), it becomes If Y(nT)'k is calculated, the oscillation output of vGO has been calculated.

第2図に式■の演算を行なうための構成を示す。FIG. 2 shows a configuration for calculating equation (2).

ココテ、v(nT)はvOOへの入力1龜号、Tけ1標
本化周期分だけψ(n’l’)’t遅延させる遅延器、
COSはコサイン変換器である。しかし、第2図のVC
Oでは発振出力y(nT)′ff:得るために.コサイ
ン変換をしなけ几ばならず、この変俟は複帷なものであ
る。
Here, v(nT) is the input signal to vOO, a delay device that delays ψ(n'l')'t by T times one sampling period,
COS is a cosine transformer. However, the VC in Figure 2
At O, the oscillation output y(nT)'ff: To obtain. A cosine transformation is necessary, and this transformation is complex.

そこで、本発B月では、発振出力.y(nT)ffi正
弦関数波形でなく三角波形として複雑な演算の必要の無
い構成とする。第3図に本発明の一実施例の構成を示す
Therefore, in the main launch month B, the oscillation output. y(nT)ffi It is configured as a triangular waveform instead of a sine function waveform and does not require complicated calculations. FIG. 3 shows the configuration of an embodiment of the present invention.

第3図において、1は所定の標本化周波数Fgで標本化
されたディジタル信号V(nT)の入力端子、2けその
人力V(n.T)に第1のディジタル係数C1を掛ける
掛算器、3は.データセレク、4は加算器、5はDタイ
プフリップフロップ(記憶器.遅延器として用いる)、
6はデコーダ、7はフリ゛)ヘプフOyプ、8ツ9はE
X−ORゲート、1oは発振出力,’/(nT)の出力
端子である。ここでは,回路構成を簡単にするために、
加算器4を1つとして、標本化周期内で2度加算1−る
ようにしている。デコーダ6への入力は点線で示さnて
おり、ここで各々の信号の符号を調べている。
In FIG. 3, 1 is an input terminal for a digital signal V (n.T) sampled at a predetermined sampling frequency Fg; 2 is a multiplier that multiplies the human power V (n.T) by a first digital coefficient C1; 3 is. Data select, 4 is adder, 5 is D type flip-flop (memory, used as delay device),
6 is a decoder, 7 is a free) Hepfu Oyp, 8 and 9 are E
The X-OR gate, 1o is the output terminal of the oscillation output, '/(nT). Here, to simplify the circuit configuration,
With one adder 4, addition is performed twice within the sampling period. The input to the decoder 6 is indicated by a dotted line n, where the sign of each signal is checked.

この回路による三角波発生の様子全第4図に示す。ここ
で扱うディンタル数値は2の補数表示(2’C)さnて
おり、その最大値を±IK正規化嘔して考える。今、第
4図で入カディジクル信号v(nT)を直流としnT=
Qで演算を開始するとする。i’l=1のときにはV(
’nT)xC1(l随では0.15)¥−データセレク
タ3で選択パルスt1により選択し、デコーダ6でその
符号ケ調べ、更にフリップフロノプ7により加算するが
減算するがを選択する(図の場合では加n:tする)。
The entire situation of triangular wave generation by this circuit is shown in FIG. The digital value handled here is represented by two's complement (2'C), and its maximum value is considered by normalizing ±IK. Now, in Fig. 4, let the input dissipicle signal v(nT) be a direct current, and nT=
Suppose we start the calculation at Q. When i'l=1, V(
'nT) Then add n:t).

こ几により、加算器4でD−フリノブフロノプ5がらの
1標本化周期前の出力y(n’r)と加算する。n二o
のと@cy(n’r.)==ofあッタとす:ltぱ、
第4図のn=iの様になる。次に、C2(図では0・4
)データセレクク3が選択されて加算される。このとき
加算器4がオーバーフローすると,デコーダlc.!:
!ll検出さnてEXffORゲ−ト9K”1′′を入
力して加算出力を反転して三角波として正しい値を出力
する(n=2の状態)。同時に、FF7によりEX−O
Rゲート8に゛1″を入力して次.の演算からは加算で
はなく減算が行なわれるようにする。これを続けると第
4図の点線の如く発振出力3/(nT)として三角波が
得られる。
According to this method, the adder 4 adds the output y(n'r) of the D-Flinob Fronop 5 one sampling period before. n2o
Noto@cy(n'r.)==ofattato:ltpa,
It becomes like n=i in FIG. Next, C2 (0.4 in the figure)
) Data select 3 is selected and added. At this time, if adder 4 overflows, decoder lc. ! :
! ll is detected, inputs EXffOR gate 9K"1'', inverts the addition output, and outputs the correct value as a triangular wave (state of n = 2). At the same time, EXffOR gate 9K"1'' is input by FF7.
Input "1" to the R gate 8 so that subtraction is performed instead of addition from the next operation.Continuing this, a triangular wave is obtained as the oscillation output 3/(nT) as shown by the dotted line in Figure 4. It will be done.

この発振器では,発振周波数Fは標本化周波数をFsと
して F=FsX(C2+V(nT)XO1)’.’/4とな
る。発振周波数の上限は/2下、下限はディジタル数値
の有効データ長によって決ま.る。
In this oscillator, the oscillation frequency F is F=FsX(C2+V(nT)XO1)', where Fs is the sampling frequency. '/4. The upper limit of the oscillation frequency is determined by /2 or lower, and the lower limit is determined by the effective data length of the digital value. Ru.

vCOとしての機能は、第退のデイジタノレ係数02に
よりVCOの中心周波数FOを与え、第1のディジタ,
,係数01によりVCOの制御感度を与えるようにする
The function as a vCO is to give the center frequency FO of the VCO by the first digit coefficient 02,
, the coefficient 01 gives the control sensitivity of the VCO.

すなわちFo=FsXCz/4となる。That is, Fo=FsXCz/4.

発明の効果 ぺのように、本発明によれば、次のような効果が得られ
る。
Effects of the Invention As described above, according to the present invention, the following effects can be obtained.

(1)入力信号の振巾と出力周波数は完全に線形である
(1) The amplitude of the input signal and the output frequency are completely linear.

(2)’VCOの中心周波数、制帥感度にディジタル係
数01,C,2i変えるだけで変えつるので簡単である
(2) It is easy to change the center frequency of the VCO and the limiting sensitivity by simply changing the digital coefficients 01, C, and 2i.

(3)周波数安定度はクアノクの周波数に依存し、..
樺めて安定である。
(3) Frequency stability depends on the quanok frequency. ..
It is stable and stable.

((ニ)複雑な演算は不必要であり、回路が瞳めて簡単
で.ある。
((d) Complex calculations are unnecessary, and the circuit is strikingly simple.

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

第1図は一般的なPLL回路のブロノク図、第2図は従
来のディジタル制御発振器のブロソク図,第31gは本
発明の一実施例におけるディジクル制御発i器のブロッ
ク図、第4図はその動作を説明するための波形図である
。 1・・・・・・入力端子、2・・・・・・掛算器、3・
・・・・・データセレクタ、4・・・・・・加算器、6
・・・・・・D−フリップフロップ、6・・・・・・デ
コーダ、7・・・・・・フリップフロップ、.8,9・
・・・・・EX−ORゲート、1o・・・・・・出力端
子。 =32
Figure 1 is a block diagram of a general PLL circuit, Figure 2 is a block diagram of a conventional digitally controlled oscillator, Figure 31g is a block diagram of a digitally controlled oscillator according to an embodiment of the present invention, and Figure 4 is its block diagram. FIG. 3 is a waveform diagram for explaining the operation. 1... Input terminal, 2... Multiplier, 3.
...Data selector, 4...Adder, 6
......D-flip-flop, 6...decoder, 7...flip-flop, . 8,9・
...EX-OR gate, 1o...Output terminal. =32

Claims (1)

【特許請求の範囲】[Claims] (1)所定の標本化周彼数で標本されたデイジタル信号
を入力とし、その入力に第1のデイジタル係数を掛け、
その積と第2のデイジタル係数02と1標本化周期前の
演算結果との3つのディジタル信号を演算手段により演
算し、その演算結果を出力するとともに、その演算結果
を次の標本化時の演算用に記憶することを特徴とするデ
ィジタル制御発振器。 2)演算手段として加減算器を設け、前記加減算器のオ
ーバーフロー出力もしくは加減算出力が加えられている
比較器の出力により鋸歯状波あるいは三角教ヲ発生させ
るように論理回路により前記加減算器の加減算制御をす
るようにしたことを%徴とする特許請求の範囲第1項記
載のディジタル制御発振器。
(1) Take as input a digital signal sampled at a predetermined number of sampling cycles, multiply the input by a first digital coefficient,
The three digital signals of the product, the second digital coefficient 02, and the calculation result from one sampling period before are calculated by the calculation means, and the calculation result is output, and the calculation result is used for the calculation at the next sampling time. A digitally controlled oscillator characterized by being memorized for use. 2) An adder/subtractor is provided as an arithmetic means, and the addition/subtraction of the adder/subtractor is controlled by a logic circuit so that a sawtooth wave or triangular wave is generated by the overflow output of the adder/subtractor or the output of a comparator to which the addition/subtraction output is applied. The digitally controlled oscillator according to claim 1, wherein the digitally controlled oscillator is characterized in that the digitally controlled oscillator is configured to have the following characteristics.
JP57130825A 1982-07-27 1982-07-27 Digital control oscillator Pending JPS5921104A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57130825A JPS5921104A (en) 1982-07-27 1982-07-27 Digital control oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57130825A JPS5921104A (en) 1982-07-27 1982-07-27 Digital control oscillator

Publications (1)

Publication Number Publication Date
JPS5921104A true JPS5921104A (en) 1984-02-03

Family

ID=15043587

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57130825A Pending JPS5921104A (en) 1982-07-27 1982-07-27 Digital control oscillator

Country Status (1)

Country Link
JP (1) JPS5921104A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0430441A2 (en) * 1989-11-17 1991-06-05 Digital Equipment Corporation Method and apparatus for correction of positive and negative overflow

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0430441A2 (en) * 1989-11-17 1991-06-05 Digital Equipment Corporation Method and apparatus for correction of positive and negative overflow

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