JPS60190019A - Frequency multiplier circuit - Google Patents

Frequency multiplier circuit

Info

Publication number
JPS60190019A
JPS60190019A JP4635984A JP4635984A JPS60190019A JP S60190019 A JPS60190019 A JP S60190019A JP 4635984 A JP4635984 A JP 4635984A JP 4635984 A JP4635984 A JP 4635984A JP S60190019 A JPS60190019 A JP S60190019A
Authority
JP
Japan
Prior art keywords
circuit
frequency
wave
waveform
points
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
JP4635984A
Other languages
Japanese (ja)
Inventor
Seiichi Igarashi
五十嵐 清一
Iwao Nakayama
中山 巖
Hideo Endo
秀男 遠藤
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.)
Matsushima Kogyo KK
Original Assignee
Matsushima Kogyo KK
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 Matsushima Kogyo KK filed Critical Matsushima Kogyo KK
Priority to JP4635984A priority Critical patent/JPS60190019A/en
Publication of JPS60190019A publication Critical patent/JPS60190019A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03KPULSE TECHNIQUE
    • H03K12/00Producing pulses by distorting or combining sinusoidal waveforms

Abstract

PURPOSE:To obtain a highly accurate multiple frequency with a small sized and inexpensive circuit by combining frequency multiplier circuits each comprising a waveform distortion circuit and a waveform shaping circuit in series or parallel. CONSTITUTION:The series connection between the waveform distortion circuit 5 and the waveform shaping circuit 6 is used as a basic building block. A distorted wave shown in Fig. B having a regular distortion is obtained from a fundamental wave A by the circuit 5 and a multiplied wave is obtained further by the waveform shaping circuit 6. In order to obtain, e.g., a two-multiple wave, a threshold value is set to a P axis in Fig. B and points (d), (e), (h), (i) are obtained as trigger points and an output is obtained from the points. In order to obtain a three-multiple wave, a threshold value is set to a Q axis and points (a), (b), (c), (f), (g), (j) are used as trigger points. Moreover, a high multiplication is obtained by connecting said multiplier circuits in series. Moreover, an optional frequency is obtained by the series connection of said multiplier circuit and a frequency division circuit and also a parallel circuit in Fig. A circuit 9 is a gate circuit.

Description

【発明の詳細な説明】 〔技術分野〕 本発明は入力波の逓倍波を得る周波数逓倍回路に関する
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to a frequency multiplier circuit that obtains a multiplied wave of an input wave.

〔従来技術〕[Prior art]

従来の逓倍波を得るため、FMステレオ副搬送波再生、
トランシーバ等に用いられている周知の同波数逓倍回路
であるP L L (Phase−Locked−LO
Op)を第1図に示す。同図において、該PLLは内部
に位相比較器1(以下、COMPl)、低域フィルタ2
(以下% L P F2 ) 、電圧制御発振器3(以
下、VC(1)、周波数分周器4(以下、DIV4)を
有する帰還系である。同図において、COMPlは入力
信号fsとvC03により電圧制御されDIV4により
 fo/N (Nは逓倍数)に分周された周波数と各々
の位相とを比較する。
To obtain the conventional multiplication wave, FM stereo subcarrier reproduction,
PLL (Phase-Locked-LO) is a well-known same wave number multiplier circuit used in transceivers etc.
Op) is shown in FIG. In the figure, the PLL includes a phase comparator 1 (hereinafter referred to as COMPl) and a low-pass filter 2.
(hereinafter referred to as % L P F2 ), a voltage controlled oscillator 3 (hereinafter referred to as VC(1)), and a frequency divider 4 (hereinafter referred to as DIV4). Each phase is compared with the controlled frequency divided into fo/N (N is a multiplier) by DIV4.

そしてその出力はLPF2を通って前記VCO3の制御
端子に加えられ、入力信号とVCO3の発振周波数差な
らびに位相差を低減する方向にVC06の周波数を変化
させる。この回路をループさせることによpfo=Nf
sが得られるものである。
The output thereof is applied to the control terminal of the VCO 3 through the LPF 2, and the frequency of the VC 06 is changed in the direction of reducing the oscillation frequency difference and phase difference between the input signal and the VCO 3. By looping this circuit, pfo=Nf
s is obtained.

以上、従来の周波数逓倍回路の欠点は、第一に構造が複
雑で小型化が困難であり、しかも高価なことである。こ
れは前述のようにCOIVf P%LPF、VCOlD
IVといった専用の集積回路(少なくとも、COMPと
LPF、VC(J%DIVの5種類)の組合せが必要で
あることから、構造を複雑化すること、部品コスト、実
装コストが高くなること、さらに小型化を困難にしてい
ることなどが原因である。第二の欠点は周波数精度が不
安定なことである。これは周波数精度が精度的に限界の
あるvCOに依存しているところに原因がある。また、
VCOの精度をより向上しようとすればさらに高価格に
ならざるを得ない。
As mentioned above, the disadvantages of the conventional frequency multiplier circuit are first that the structure is complicated, making it difficult to miniaturize, and moreover, it is expensive. As mentioned above, this is COIVf P%LPF, VCOld
Since a dedicated integrated circuit such as IV (at least a combination of COMP, LPF, and VC (J%DIV)) is required, the structure is complicated, component costs and mounting costs are high, and the size is small. The second drawback is that frequency accuracy is unstable.This is due to the fact that frequency accuracy depends on vCO, which has a limited accuracy. .Also,
If the precision of the VCO is to be further improved, the price will inevitably become even higher.

〔目 的〕〔the purpose〕

本発明はこのような問題点を解決するもので、その目的
とするところは、高精度な逓倍周波数の得られる安価で
小型な周波数逓倍回路を提供することにある。
The present invention is intended to solve these problems, and its purpose is to provide an inexpensive and compact frequency multiplication circuit that can obtain a highly accurate multiplication frequency.

〔概 要〕〔overview〕

入力する周波数の波形を規則的に歪ませる波形歪回路と
、該歪波形回路によシ規則的な歪みを有る波形を入力波
の周波数の逓倍に得る波形整形回路とで構成する周波数
逓倍回路を直列または並列に組合せたことを特徴とする
周波数逓倍回路。
A frequency multiplier circuit comprising a waveform distortion circuit that regularly distorts the waveform of an input frequency, and a waveform shaping circuit that obtains a regularly distorted waveform by multiplying the frequency of the input wave by the distorted waveform circuit. A frequency multiplier circuit characterized by being combined in series or in parallel.

〔実施例〕 本発明の詳細な説明に入る前に本発明の背景についてま
ず説明する。
[Example] Before entering into the detailed description of the present invention, the background of the present invention will be explained first.

周知のように、水晶振動子等の圧電振動子を発振回路に
より共抛周波数で発振させた場合、第2図(A)の波形
のような基本波(正弦波)を示す。
As is well known, when a piezoelectric resonator such as a crystal resonator is caused to oscillate at a resonant frequency by an oscillation circuit, it exhibits a fundamental wave (sine wave) as shown in the waveform of FIG. 2(A).

この基本波をバイアスをかけないコンプリメンタリ−回
路等の増巾器に入力させると第2図(B)のような波形
を示すことも周知である。この波形はひずみ波であり通
常は極力排除し、いかにして基本波に近ずけるかに技術
的努力が払われている。
It is also well known that when this fundamental wave is inputted to an amplifier such as a complementary circuit which is not biased, a waveform as shown in FIG. 2(B) is obtained. This waveform is a distorted wave, and technical efforts are usually made to eliminate it as much as possible and make it as close to the fundamental wave as possible.

ところが、本発明はこのひずみ波を逆に利用することに
よシ極めて容易に、しかも高精度で安価に逓倍波を得ら
れることを確かめることができだ6゜本発明はそのだめ
の周波数逓倍回路であり、以下実施例にもとすき詳細に
説明する。
However, the present invention has been able to confirm that by inversely utilizing this distorted wave, a multiplied wave can be obtained extremely easily, with high precision, and at low cost. This will be explained in detail in the following examples.

第3図は本発明の実施例を示すブロック図であり、入力
する周波数fsの波形を規則的にひずませる波形ひずみ
回路5と、該波形ひずみ回路5により規則的なひずみを
有する波形を入力波の周波数f8のN倍の周波数N f
 sを得る波形整形回路6とで構成されるものである。
FIG. 3 is a block diagram showing an embodiment of the present invention, which includes a waveform distortion circuit 5 that regularly distorts a waveform of an input frequency fs, and a waveform that has regular distortion by the waveform distortion circuit 5. The frequency N f which is N times the frequency f8 of
s.

以上本例によって得られる逓倍波について第4図の波形
図にもとすいで説明する。
The multiplied wave obtained by this example will now be explained with reference to the waveform diagram of FIG. 4.

同図(A)は第2図(A)と同様の基本波で正弦波を示
し、同図(B)はひずみ波であるが本例の説明を容易に
するために第2図(B)のひずみ波と少し波形を異にし
て示しである。従来例でも説明したように、第4図(B
)に示すひずみ波はたとえば増rIJ器等の過増巾によ
り生じることは周知であり。
Figure 2 (A) shows a sine wave with the same fundamental wave as Figure 2 (A), and Figure 2 (B) shows a distorted wave, but for ease of explanation of this example, Figure 2 (B) This is a slightly different waveform from the distorted wave. As explained in the conventional example, Fig. 4 (B
It is well known that the distorted waves shown in ) are caused by over-amplification, such as in an IJ amplifier.

本発明の波形ひずみ回路5もこれを用いている。The waveform distortion circuit 5 of the present invention also uses this.

本例は、該波形ひずみ回路5により規則的にひずみを有
する第4図(B)のひずみ波を波形整形回路乙によシ得
られる逓倍波(2〜n倍波)の−例として、同図(C)
に2倍波を、同図(D)に3倍波を各々示す。同図(C
)の2倍波を得るためには、同図(B)のP軸にしきい
値を設定し、トリガー点としてd、e、h、fおよび1
% o、r、a・・・・・・を得、とのトリガー点にお
いて出力させればよい。
In this example, the distorted wave shown in FIG. 4(B) which is regularly distorted by the waveform distortion circuit 5 is used as an example of a multiplied wave (2nd to nth harmonic wave) obtained by the waveform shaping circuit B. Diagram (C)
2 shows the second harmonic wave, and (D) shows the third harmonic wave. The same figure (C
), set a threshold on the P axis in the same figure (B), and use d, e, h, f and 1 as trigger points.
% o, r, a... can be obtained and output at the trigger point.

同様にして同図(D)の3倍波を得るためには、同図(
B)のQ軸にしきい値を設定し、トリガー点としてのa
s bs Cs fs gs Jおよびに、l、m。
Similarly, in order to obtain the third harmonic wave shown in (D) in the same figure,
Set a threshold on the Q axis of B) and set a as the trigger point.
s bs Cs fs gs J and to, l, m.

p、q% L・・・・・・を得、2倍波同様このトリガ
ー点において出力させれば良い。なお、本発明に用いる
波形ひずみ回路5は本例ではバイアスをかけないコンプ
リメンタリ−回路等の増巾器により説明したが、以上の
説明でも明らかなように規則的なひずみ波が得られる波
形ひずみ回路でおれば本発明の実施は可能である。また
、波形整形回路6は波形を任意のレベルにしきい値を設
定しトリガー点を得、出力できるものであれば本発明の
実施ゆ、可能であり、本出願人は増1】器または比較器
またはゲート回路を用いて前述の逓倍波を得ている。
It is sufficient to obtain p, q% L... and output it at this trigger point in the same way as the second harmonic wave. In this example, the waveform distortion circuit 5 used in the present invention has been explained using an amplifier such as a complementary circuit that does not apply bias, but as is clear from the above explanation, it is a waveform distortion circuit that can obtain regular distorted waves. If so, the present invention can be implemented. In addition, the waveform shaping circuit 6 can be used to implement the present invention as long as it can set a threshold value for the waveform at an arbitrary level, obtain a trigger point, and output the signal. Alternatively, the above-mentioned multiplied wave is obtained using a gate circuit.

なお、本例では逓倍波として2倍、6倍波を敗り」した
が、第5図(B)のひずみ波を変化させることにより任
意の逓倍波を得ることが可能である。
In this example, the 2nd and 6th harmonic waves are used as the multiplied waves, but any multiplied wave can be obtained by changing the distorted wave shown in FIG. 5(B).

第5図は以上に説明した周波数逓倍回路(以下。FIG. 5 shows the frequency multiplier circuit (hereinafter referred to as "the frequency multiplier circuit") explained above.

逓倍回路)7を2段以上直列に接続した実施例であり、
各々の逓倍回路7a〜7nの逓倍量の段数倍の周波数が
得られるものである。たとえば、同図において第1段目
の逓倍回路で2倍、第2段目の逓倍回路で5倍、第3段
目の逓倍回路で2倍にそれぞれ増1Jすれば、人力周波
数fsは第1段目で2fs、第2段目で6fs1第6段
目で12 fsと出力することになり、同図のようにn
段接続した場合にはその段数倍の出力が得られることに
なる。
This is an embodiment in which two or more stages of multiplier circuits) 7 are connected in series,
A frequency that is multiplied by the number of stages of the multiplication amount of each of the multiplier circuits 7a to 7n can be obtained. For example, in the figure, if the first-stage multiplier circuit doubles, the second-stage multiplier circuit multiplies five times, and the third-stage multiplier circuit doubles by 1J, the human frequency fs becomes the first The output will be 2 fs at the 2nd stage, 6 fs at the 2nd stage, and 12 fs at the 6th stage, as shown in the figure.
If stages are connected, the output will be multiplied by the number of stages.

第6図は逓倍回路7”と分周回路8とを接続した他の実
施例であり、入力周波数をfs1逓倍回路7゜の逓倍数
を5倍、分周回路8の分周段を1/2とした場合1.5
・fsの出力が得られる構成金示すものである。この構
成は、第5図と組合せることにより任意の周波数出力を
選択することが可能である。
FIG. 6 shows another embodiment in which a multiplier circuit 7'' and a frequency divider circuit 8 are connected, and the input frequency is multiplied by 5 times the input frequency of the fs1 multiplier circuit 7°, and the frequency division stage of the frequency divider circuit 8 is set to 1/1. 1.5 when set to 2
・It shows the component that can obtain the fs output. By combining this configuration with FIG. 5, it is possible to select an arbitrary frequency output.

さらに第7図に、第5図の実施例と第6図の実施例を並
列に接続し、ゲート回路9により混合させる構成を示す
Further, FIG. 7 shows a configuration in which the embodiment of FIG. 5 and the embodiment of FIG. 6 are connected in parallel and mixed by a gate circuit 9.

〔効 果〕〔effect〕

1、 本発明の周波数逓倍回路は、安定な増巾率を有す
る波形ひずみ回路と、安定したしきい値の得られる波形
整形回路との組合せにより逓倍波の周波数の出力が得ら
れるため、極めて高精度な逓倍波を提供することができ
る。
1. The frequency multiplier circuit of the present invention can output the frequency of the multiplied wave by combining a waveform distortion circuit with a stable amplification factor and a waveform shaping circuit with a stable threshold value, so it can produce an extremely high frequency output. Accurate multiplication waves can be provided.

2、 波形ひずみ回路と波形整形回路だけの簡易な構成
のため、集積回路で1種類に実装できることから、部品
コスト、実装コストを大巾に低減することが可能となシ
小型化も実現できる。
2. Due to the simple configuration of only a waveform distortion circuit and a waveform shaping circuit, it can be implemented as a single type of integrated circuit, making it possible to significantly reduce component costs and mounting costs, and achieve miniaturization.

五 本発明の周波数逓倍回路は、直列接続により、高い
倍率の故波数逓倍が可能であり、更に、従来の分周器と
の直列接続、および、ケート回路を利用した並列接続を
行なうことにより、自在な周波数逓倍量を得ることがで
きる。このため、たとえば32KHzの時計用発振器に
よって2〜6 Ml(zのマイコン用の温償を得ること
、および2 MHzの温償から3−5MHzの温償を得
ること等が容易にi」能となり、その応用範囲は非常に
広いものである。
5. The frequency multiplier circuit of the present invention is capable of high frequency multiplication by series connection, and furthermore, by series connection with a conventional frequency divider and parallel connection using a gate circuit, A flexible amount of frequency multiplication can be obtained. For this reason, for example, it is easily possible to obtain temperature compensation for a microcontroller of 2 to 6 Ml (z) using a 32 KHz clock oscillator, and to obtain temperature compensation of 3-5 MHz from temperature compensation of 2 MHz. , its application range is extremely wide.

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

第1図は従来例のブロック図 第2図は波形図を示し、同図(A)は基本波、同図(B
)はひずみ波、 第6図は本発明の実施例を示すブロック図、第5図は本
発明の1実施例を示すブロック図第6図は本発明の1実
施例を示すブロック図第7図は本発明の他の実施例を示
すブロック図5は波形ひずみ回路 6は波形整形回路以
上 矛2図 矛3周 1−(SeC) +4 回
Figure 1 is a block diagram of a conventional example. Figure 2 is a waveform diagram, in which (A) shows the fundamental wave and (B)
) is a distorted wave. FIG. 6 is a block diagram showing an embodiment of the present invention. FIG. 5 is a block diagram showing one embodiment of the present invention. FIG. 6 is a block diagram showing one embodiment of the present invention. is a block diagram showing another embodiment of the present invention. 5 is a waveform distortion circuit. 6 is a waveform shaping circuit.

Claims (1)

【特許請求の範囲】[Claims] 入力する周波数の波形を規則的にひずませる波形ひずみ
回路と、該波形ひずみ回路により規則的なひずみを有す
る波形を入力波の周波数の逓倍に得る波形整形回路とで
構成する周波数逓倍回路を直列または並列に組合せたこ
とを特徴とする周波数逓倍回路。
A frequency multiplier circuit consisting of a waveform distortion circuit that regularly distorts the waveform of the input frequency and a waveform shaping circuit that obtains a regularly distorted waveform by multiplying the frequency of the input wave by the waveform distortion circuit is connected in series or A frequency multiplier circuit characterized by being combined in parallel.
JP4635984A 1984-03-09 1984-03-09 Frequency multiplier circuit Pending JPS60190019A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4635984A JPS60190019A (en) 1984-03-09 1984-03-09 Frequency multiplier circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4635984A JPS60190019A (en) 1984-03-09 1984-03-09 Frequency multiplier circuit

Publications (1)

Publication Number Publication Date
JPS60190019A true JPS60190019A (en) 1985-09-27

Family

ID=12744954

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4635984A Pending JPS60190019A (en) 1984-03-09 1984-03-09 Frequency multiplier circuit

Country Status (1)

Country Link
JP (1) JPS60190019A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011049420A (en) * 2009-08-28 2011-03-10 Tdk Corp Coil component

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011049420A (en) * 2009-08-28 2011-03-10 Tdk Corp Coil component
US8253522B2 (en) 2009-08-28 2012-08-28 Tdk Corporation Coil component having wire-support member

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