JPS6125038Y2 - - Google Patents

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Publication number
JPS6125038Y2
JPS6125038Y2 JP9394379U JP9394379U JPS6125038Y2 JP S6125038 Y2 JPS6125038 Y2 JP S6125038Y2 JP 9394379 U JP9394379 U JP 9394379U JP 9394379 U JP9394379 U JP 9394379U JP S6125038 Y2 JPS6125038 Y2 JP S6125038Y2
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JP
Japan
Prior art keywords
voltage
diode
connection point
resistor
capacitor
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.)
Expired
Application number
JP9394379U
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Japanese (ja)
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JPS5613295U (en
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Filing date
Publication date
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Priority to JP9394379U priority Critical patent/JPS6125038Y2/ja
Publication of JPS5613295U publication Critical patent/JPS5613295U/ja
Application granted granted Critical
Publication of JPS6125038Y2 publication Critical patent/JPS6125038Y2/ja
Expired legal-status Critical Current

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Description

【考案の詳細な説明】 本考案は第1の効果用任意の電圧E2によりピ
アノ音や打楽器音等のいわゆるパーカツシヨン効
果のエンベロープと、通常の楽音信号のエンベロ
ープとを任意に合成または連続して可変せしめ、
第2の効果用任意の電圧E3により上記第1の効
果用任意の電圧E2によつて得られたエンベロー
プにサステイン効果の長さを任意に可変し付加せ
しめることができる電子楽器のエンベロープ発生
装置に関する。
[Detailed description of the invention] The present invention uses a first arbitrary voltage E2 for effect to arbitrarily synthesize or continuously combine the envelope of a so-called percussion effect such as a piano sound or percussion instrument sound with the envelope of a normal musical sound signal. variable limit,
Envelope generation for an electronic musical instrument in which the length of a sustain effect can be arbitrarily varied and added to the envelope obtained by the above-mentioned first effect voltage E 2 using an arbitrary voltage E 3 for a second effect. Regarding equipment.

本考案の一実施例を第1図に示し以下に詳細に
説明する。
An embodiment of the present invention is shown in FIG. 1 and will be described in detail below.

すなわち、鍵スイツチK1の一方を電源E1に接
続し、他方を直列に接続した第1のコンデンサ
C1と第1のダイオードD1とを介して緩衝器A1
接続し、鍵スイツチK1と第1のコンデンサC1
の接続点Aと、第1のコンデンサC1と第1のダ
イオードD1との接続点Bとを直列に接続した第
1の抵抗器R1と第2のダイオードD2とを介して
接続し、第1の抵抗器R1と第2のダイオードD2
との接続点に第3のダイオードD3を介して第1
の効果用の任意の電圧E2を接続し、第1のダイ
オードD1と緩衝器A1との接続点と接地レベルに
第2のコンデンサC2と第2の抵抗器R2とを並列
に接続し、さらに第1のダイオードD1と緩衝器
A1との接続点Gに第3の抵抗器R3と第4のダイ
オードD4とを介して第2の効果用の任意の電圧
E3を直列に接続してなる。
That is, one side of the key switch K 1 is connected to the power source E 1 , and the other side is connected in series with the first capacitor.
C 1 and the first diode D 1 to the buffer A 1 , and the connection point A between the key switch K 1 and the first capacitor C 1 and the first capacitor C 1 and the first diode. The connection point B with D 1 is connected through a first resistor R 1 and a second diode D 2 connected in series, and the first resistor R 1 and the second diode D 2 are connected in series.
the first through the third diode D 3 at the connection point with
Connect an arbitrary voltage E 2 for the effect of , and connect the second capacitor C 2 and the second resistor R 2 in parallel to the connection point of the first diode D 1 and the buffer A 1 and the ground level. Connect and further buffer with the first diode D 1
An arbitrary voltage for the second effect is applied to the connection point G with A 1 through the third resistor R 3 and the fourth diode D 4
It is formed by connecting E 3 in series.

上記構成において、第1の電圧E2と第2の電
圧E3がともに接地レベルの場合、第1の抵抗器
R1と第2のダイオードD2との接続点は第3のダ
イオードD3を介して接地レベルとなり、第3の
抵抗器R3は第4のダイオードD4を介して接地レ
ベルに接続され、第1のコンデンサC1、第2の
抵抗器R2、第3の抵抗器R3で微分回路が構成さ
れるので、鍵スイツチK1が第2図Aの区間t1で示
される様にON,OFFされると接続点Bには第2
図B1の区間t1で示される様な微分回路の時定数τ
で減衰する電圧が現われ、該電圧が第1のダイ
オードD1を介して接続点Gに伝えられるので、
該接続点Gの電圧波形は第2図G1の区間t1′で示
される様になり、緩衝器A1を介して出力V0には
第2図G1の区間t1′で示されるエンベロープ電圧
波形が現われ、パーカツシヨン効果のエンベロー
プが得られるものである。
In the above configuration, if the first voltage E 2 and the second voltage E 3 are both at ground level, the first resistor
The connection point between R 1 and the second diode D 2 is connected to the ground level via the third diode D 3 , and the third resistor R 3 is connected to the ground level via the fourth diode D 4 . The first capacitor C 1 , the second resistor R 2 , and the third resistor R 3 constitute a differential circuit, so the key switch K 1 is turned ON as shown in section t 1 of FIG. 2A. , when turned OFF, the second
Time constant τ of a differentiator circuit as shown in interval t 1 in Figure B 1
Since a voltage appears that decays at 1 and is transmitted through the first diode D 1 to the connection point G,
The voltage waveform at the connection point G becomes as shown in the section t 1 ' in FIG. 2 G 1 , and the voltage waveform at the output V 0 via the buffer A 1 is shown in the section t 1 ' in FIG. 2 G 1 . An envelope voltage waveform appears and the envelope of the percussion effect is obtained.

次に、第1の電圧E2を例えば電源E1の1/2の電
圧とし、第2の電圧E3が接地レベルの状態で鍵
スイツチK1をONすると、第1の抵抗器R1と第2
のダイオードD2との接続点の電圧は第3のダイ
オードD3を介してほぼ電源E1の1/2の電圧とな
り、電源E1の1/2の電圧より低に電圧以下の電圧
では第1の抵抗器R1と第2のダイオードD2を介
して接続点Aと接続点Bは導通常態となるため、
接続点Bには前記時定数τで減衰した後、電源
E1の1/2の電圧で一定となる電圧波形が現われ、
第1のダイオードD1を介して接続点Gに伝えら
れる。次に、鍵スイツチK1をOFFすると、接続
点A及び接続点Bはすぐに接地レベルとなるが、
接続点Gは第2のコンデンサC2の働きによりす
ぐに接地レベルとはならず、第2のコンデンサ
C2、第2の抵抗器R2、第3の抵抗器R3で構成さ
れる放電回路の時定数τで減衰する電圧波形と
なる。よつて、鍵スイツチK1のON,OFFに伴い
接続点Gには第2図G1の区間t2′で示される電圧
波形が現われ、出力V0には緩衝器A1を介して接
続点Gの電圧波形と同様のエンベロープ電圧波形
が現われる。
Next, when the first voltage E 2 is set to, for example, 1/2 of the voltage of the power supply E 1 and the key switch K 1 is turned on with the second voltage E 3 at the ground level, the first resistor R 1 and Second
The voltage at the connection point with diode D 2 becomes approximately 1/2 of the voltage of the power supply E 1 through the third diode D 3 , and at a voltage lower than 1/2 of the voltage of the power supply E 1 , Since the connection point A and the connection point B become conductive through the first resistor R1 and the second diode D2 ,
After attenuating with the time constant τ 1 , the power supply is connected to the connection point B.
A voltage waveform that is constant at 1/2 of E 1 appears,
It is transmitted to the connection point G via the first diode D1 . Next, when key switch K1 is turned OFF, connection point A and connection point B immediately go to the ground level, but
The connection point G does not reach the ground level immediately due to the action of the second capacitor C2 .
C 2 , the second resistor R 2 , and the third resistor R 3 form a voltage waveform that attenuates with the time constant τ 2 of the discharge circuit. Therefore, as the key switch K1 turns ON and OFF , a voltage waveform shown in section t2 ' in FIG. An envelope voltage waveform similar to the voltage waveform of G appears.

すなわち、前記パーカツシヨン効果と通常の楽
音信号とのエンベロープが合成されたエンベロー
プが得られるものである。
That is, an envelope is obtained in which the envelopes of the percussion effect and the normal musical tone signal are synthesized.

次に、第1の電圧E2を電源E1と同一電圧と
し、第2の電圧E3を接地レベルとした状態で鍵
スイツチK1をONすると、第1の抵抗器R1と第2
のダイオードD2との接続点の電圧は第3のダイ
オードD3を介してほぼ電源E1と同一電圧とな
り、接続点Aと接続点Bは第1の抵抗器R1と第
2のダイオードD2を介して導通常態となるの
で、接続点Gには第1のダイオードD1を介して
ほぼ電源E1と同一電圧が現われる。次に、鍵ス
イツチをOFFにすると、前記同様接続点Bの電
圧はすぐに接地レベルになるが、第2のコンデン
サC2の働きにより接続点Gには前記時定数τ
で減衰する電圧波形が現われる。よつて鍵スイツ
チK1のON,OFFに伴い前記接続点Gには第2図
G1の区間t3′で示される電圧波形が現われ、出力
V0には緩衝器A1を介して接続点Gの電圧波形と
同様のエンベロープ電圧波形が現われ、前記通常
の楽音信号のエンベロープが得られるものであ
る。
Next, when the key switch K 1 is turned on with the first voltage E 2 set to the same voltage as the power supply E 1 and the second voltage E 3 set to the ground level, the first resistor R 1 and the second
The voltage at the connection point with the diode D2 becomes almost the same voltage as the power supply E1 through the third diode D3 , and the connection point A and the connection point B are connected to the first resistor R1 and the second diode D. 2 becomes conductive, so that a voltage approximately equal to that of the power source E 1 appears at the connection point G via the first diode D 1 . Next, when the key switch is turned OFF, the voltage at the connection point B immediately goes to the ground level as described above, but due to the action of the second capacitor C2 , the voltage at the connection point G has the above-mentioned time constant τ 2
A voltage waveform appears that attenuates at . Therefore, as the key switch K1 turns ON and OFF, the connection point G is connected to the
A voltage waveform shown in interval t 3 ′ of G 1 appears, and the output
An envelope voltage waveform similar to the voltage waveform at the connection point G appears at V0 via the buffer A1 , and the envelope of the normal musical tone signal is obtained.

次に、前記第2の電圧E3による効果を以下に
詳細に説明する。
Next, the effect of the second voltage E3 will be explained in detail below.

第1図において、接続点Bと接続点Gとは第1
のダイオードD1により一方向性を有する接続に
なつているため、接続点Bの電圧は第1のダイオ
ードD1を介して第2のコンデンサC2にすぐに充
電されるが、該電圧の放電回路は第2の抵抗器
R2、第3の抵抗器R3、第4のダイオードD4、第
2の電圧E3により形成されているから、接続点
Gの電圧は第2の電圧E3の電圧レベルまで第2
の抵抗器R2、第3の抵抗器R3、第4のダイオー
ドD4により放電され、接続点Gには前記時定数
τで減衰する電圧波形が現われるが、接続点G
の電圧が第2の電圧E3より低くなると、第4の
ダイオードD4の働きにより前記放電回路より第
3の抵抗器R3が切り放され、第2の抵抗器R2
みにより放電が行なわれるので、第2のコンデン
サC2と第2の抵抗器R2とで形成される時定数τ
で減衰する電圧波形が接続点Gに現われ、該電
圧波形は緩衝器A1を介して出力V0にサステイン
効果のエンベロープ電圧波形として得られるもの
である。
In Fig. 1, connection point B and connection point G are the first
Since the connection is unidirectional by the diode D 1 of The circuit is the second resistor
R 2 , the third resistor R 3 , the fourth diode D 4 , and the second voltage E 3 , the voltage at the connection point G reaches the voltage level of the second voltage E 3 .
is discharged by the resistor R 2 , the third resistor R 3 , and the fourth diode D 4 , and a voltage waveform that attenuates with the time constant τ 2 appears at the connection point G.
When the voltage becomes lower than the second voltage E3 , the third resistor R3 is disconnected from the discharge circuit by the action of the fourth diode D4 , and discharge is performed only by the second resistor R2. Therefore, the time constant τ formed by the second capacitor C 2 and the second resistor R 2
A voltage waveform which is attenuated by 3 appears at the connection point G, and this voltage waveform is obtained as a sustain effect envelope voltage waveform at the output V0 via the buffer A1.

すなわち、サステイン効果の時間が第2の電圧
E3により前記時定数τより時定数τに連続
して可変せしめられるものである。
In other words, the sustain effect time is equal to the second voltage.
The time constant τ 2 can be continuously varied from the time constant τ 2 to the time constant τ 3 by E 3 .

また、前記パーカツシヨン効果のエンベロープ
時定数を形成する微分回路の時定数τも同様
に、第2の電圧E3の電圧レベルより低くなる部
分では第1のコンデンサC1と第2の抵抗器R2
で形成される時定数τに変化する。
Similarly, the time constant τ 1 of the differentiating circuit that forms the envelope time constant of the percussion effect is lower than the voltage level of the second voltage E 3 between the first capacitor C 1 and the second resistor R. The time constant formed by 2 and τ changes to 4 .

すなわち、前記パーカツシヨン効果の時間も、
第2の電圧E3により前記時定数τより時定数
τに連続して可変せしめられることができるの
であり、第2図G2にエンベロープ電圧の波形例
を示すものである。
That is, the time of the percussion effect is also
The time constant τ 1 can be continuously varied from the time constant τ 1 to the time constant τ 4 by the second voltage E 3 , and an example of the waveform of the envelope voltage is shown in FIG. 2 G 2 .

尚、第2図G2において点線部で示される例
は、第2の電圧E3が電源E1の1/2の電圧の時で、
実線部は電源E1と同一電圧の時である。
In addition, the example shown by the dotted line in FIG. 2 G2 is when the second voltage E3 is 1/2 the voltage of the power source E1 ,
The solid line part is when the voltage is the same as that of the power supply E1 .

また、緩衝器A1は出力V0に接続される回路と
し、本考案のエンベロープ発生装置とが相互に干
渉しない様にするものである。
Further, the buffer A 1 is a circuit connected to the output V 0 to prevent interference between the buffer A 1 and the envelope generator of the present invention.

以上の説明のように、本考案は第1の効果用任
意の電圧E2によりパーカツシヨン効果のエンベ
ロープと通常の楽音信号のエンベロープとを任意
に合成または連続して可変せしめ、第2の効果用
任意の電圧E3により上記任意に得られたエンベ
ロープにサステイン効果の長さを任意に可変し付
加せしめるものである。
As explained above, in the present invention, the envelope of the percussion effect and the envelope of the normal musical tone signal can be arbitrarily synthesized or continuously varied by the arbitrary voltage E2 for the first effect, and The length of the sustain effect can be arbitrarily varied and added to the arbitrarily obtained envelope using the voltage E3 .

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

第1図は本考案の一実施例を示す回路図、第2
図はその動作を示す波形図である。 図面中、E1は電源、E2,E3は効果用電圧、K1
は鍵スイツチ、R1,R2,R3は抵抗、C1,C2はコ
ンデンサ、D1,D2,D3,D4はダイオード、A1
緩衝器である。
Figure 1 is a circuit diagram showing one embodiment of the present invention;
The figure is a waveform diagram showing the operation. In the drawing, E 1 is the power supply, E 2 and E 3 are the effect voltages, and K 1
is a key switch, R 1 , R 2 , R 3 are resistors, C 1 , C 2 are capacitors, D 1 , D 2 , D 3 , D 4 are diodes, and A 1 is a buffer.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 鍵スイツチK1の一方を電源E1に接続し、他方
を直列に接続した第1のコンデンサC1と第1の
ダイオードD1とを介して緩衝器A1に接続し、鍵
スイツチK1と第1のコンデンサC1との接続点と
第1のコンデンサC1と第1のダイオードD1との
接続点とを直列に接続した第1の抵抗器R1と第
2のダイオードD2とを介して接続し、第1の抵
抗器R1と第2のダイオードD2との接続点に第3
のダイオードD3を介して第1の効果用の任意の
電圧E2を接続し、第1のダイオードD1と緩衝器
A1との接続点と接地レベル間に第2のコンデン
サC2と第2の抵抗器R2とを並列に接続し、さら
に第3の抵抗器R3と第4のダイオードD4とを介
して第2の効果用の任意の電圧E3を直列に接続
してなる電子楽器のエンベロープ発生装置。
One end of the key switch K 1 is connected to the power supply E 1 , and the other end is connected to the buffer A 1 via a first capacitor C 1 and a first diode D 1 connected in series . A first resistor R1 and a second diode D2 are connected in series between the connection point with the first capacitor C1 and the connection point between the first capacitor C1 and the first diode D1. A third resistor is connected to the connection point of the first resistor R 1 and the second diode D 2 .
Connect any voltage E 2 for the first effect through the diode D 3 of the buffer with the first diode D 1
A second capacitor C 2 and a second resistor R 2 are connected in parallel between the connection point with A 1 and the ground level, and a third resistor R 3 and a fourth diode D 4 are connected in parallel. An envelope generator for an electronic musical instrument, in which an arbitrary voltage E3 for a second effect is connected in series.
JP9394379U 1979-07-06 1979-07-06 Expired JPS6125038Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9394379U JPS6125038Y2 (en) 1979-07-06 1979-07-06

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9394379U JPS6125038Y2 (en) 1979-07-06 1979-07-06

Publications (2)

Publication Number Publication Date
JPS5613295U JPS5613295U (en) 1981-02-04
JPS6125038Y2 true JPS6125038Y2 (en) 1986-07-28

Family

ID=29326837

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9394379U Expired JPS6125038Y2 (en) 1979-07-06 1979-07-06

Country Status (1)

Country Link
JP (1) JPS6125038Y2 (en)

Also Published As

Publication number Publication date
JPS5613295U (en) 1981-02-04

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