JPH0651002A - Adding circuit for electric power measuring value - Google Patents

Adding circuit for electric power measuring value

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Publication number
JPH0651002A
JPH0651002A JP4222070A JP22207092A JPH0651002A JP H0651002 A JPH0651002 A JP H0651002A JP 4222070 A JP4222070 A JP 4222070A JP 22207092 A JP22207092 A JP 22207092A JP H0651002 A JPH0651002 A JP H0651002A
Authority
JP
Japan
Prior art keywords
power
output
operational amplifier
resistance
measuring parts
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
Application number
JP4222070A
Other languages
Japanese (ja)
Other versions
JP3199284B2 (en
Inventor
Makoto Kudo
真 工藤
Kyoichi Koyama
恭市 小山
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.)
Hioki EE Corp
Original Assignee
Hioki EE 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 Hioki EE Corp filed Critical Hioki EE Corp
Priority to JP22207092A priority Critical patent/JP3199284B2/en
Publication of JPH0651002A publication Critical patent/JPH0651002A/en
Application granted granted Critical
Publication of JP3199284B2 publication Critical patent/JP3199284B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To eliminate restriction on the range setting through attainment of a correct adding result by furnishing the resistance at each output with a resistance element for changing over whose resistance value is selectively controlled in reverse proportion to the electric power range to be set on power measuring parts. CONSTITUTION:Because the output voltages V1-V3 of electric power measuring parts 11-13 are all emitted in one volt, switches S1-S5 are opened and closed on the basis of a control signal given by a control part 18 so that a resistance value in reverse proportion to the power range set on the measuring parts 11-13 is obtained among resistance elements Ra-Re for changing over at the corresponding resistances R1-R3, and thereby the resistance element which becomes effective is selected. Among the power ranges set on the measuring parts 11-13 in currently service, therefore, the addition output with the max. range made full scale relatively is always acquired at an addition power output terminal T3. In whichever combination the power range set condition on the measuring parts 11-13 is, a correct adding result is obtained at all times, and restriction on the power range setting on the measuring parts 11-13 can be eliminated.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は電力測定値の加算回路
に係り、さらに詳しくは、複数個の電力測定部を有する
ディジタルACメータなどのようなディジタル電力計に
おける電力測定値の加算回路に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a circuit for adding measured power values, and more particularly to a circuit for adding measured power values in a digital power meter such as a digital AC meter having a plurality of power measuring units.

【0002】[0002]

【従来の技術】ディジタルACメータなどのようなディ
ジタル電力計は、主として低周波交流の電力、電力量、
電圧、電流などを測定し、ディジタル表示するものであ
り、単相電力だけが測定できるものから、三相3線式、
三相4線式の三相電力をも測定することができるものま
である。
2. Description of the Related Art A digital power meter such as a digital AC meter is mainly used for low-frequency AC power, power amount,
It measures voltage, current, etc., and displays them digitally. Since only single-phase power can be measured, three-phase three-wire system,
Some even measure three-phase four-wire three-phase power.

【0003】図2は、3つの電力測定部を有して単相電
力のみならず、三相3線式、三相4線式の三相電力をも
測定することができるディジタル電力計が従来から採用
している電力測定値の加算回路の一例を示すものであ
る。
FIG. 2 shows a conventional digital power meter having three power measuring units capable of measuring not only single-phase power but also three-phase three-wire and three-phase four-wire three-phase power. 2 shows an example of an addition circuit of measured power values adopted by

【0004】同図によれば、電力測定値の加算回路の全
体は、それぞれが電圧入力端子T1と電流入力端子T2
とを各別に備えてなる3つの電力測定部1,2,3と、
これら電力測定部1,2,3からの各出力が直列接続さ
れたそれぞれの抵抗R1,R2,R3を経て反転入力端
子の側に入力されている第1オペアンプ4と、この第1
オペアンプ4からの出力が直列接続された抵抗R5を経
て反転入力端子の側に入力され、その出力側に加算電力
の出力端子T3を備えてなる第2オペアンプ5とで構成
され、第1オペアンプ4には抵抗R4により形成される
負帰還回路6が、第2オペアンプ5には抵抗R6により
形成される負帰還回路7がそれぞれ設けられている。
According to the figure, the whole of the adder circuit for the measured power values has a voltage input terminal T1 and a current input terminal T2, respectively.
And three electric power measurement units 1, 2, and 3, which are respectively provided with
A first operational amplifier 4 in which the outputs from the power measuring units 1, 2 and 3 are input to the inverting input terminal side via resistors R1, R2 and R3 connected in series, and the first operational amplifier 4
The output from the operational amplifier 4 is input to the side of the inverting input terminal via the resistor R5 connected in series, and is configured with the second operational amplifier 5 including the output terminal T3 of the added power on the output side thereof. Is provided with a negative feedback circuit 6 formed by a resistor R4, and the second operational amplifier 5 is provided with a negative feedback circuit 7 formed by a resistor R6.

【0005】なお、説明の都合上、同図中の各抵抗相互
の関係は、R1=R2=R3=3×R4であって、R5
=R6とし、各電力測定部1,2,3の電力レンジは、
そのいずれもが1000W(フルスケール)に設定され
ており、各電力測定部1,2,3の出力は、測定電力に
比例した直流電圧であり、ここでは、電力レンジのフル
スケール(1000W)に対し1Vであるとする。
For the sake of convenience of description, the relationship between the resistors in the figure is R1 = R2 = R3 = 3 × R4, and R5
= R6, the power range of each power measuring unit 1, 2, 3 is
All of them are set to 1000 W (full scale), and the output of each of the power measuring units 1, 2, and 3 is a DC voltage proportional to the measured power. Here, in the power range full scale (1000 W). On the other hand, it is assumed to be 1V.

【0006】この場合、各電力測定部1,2,3の測定
電力がそれぞれ1000W(フルスケール)のとき、電
力測定部1,2,3の出力はそれぞれ1Vとなり、第1
オペアンプ4の出力側の電圧Vaは次式により求められ
る。 Va=−(1V×R4/R1+1V×R4/R2+1V×R4/R3)=−1V
In this case, when the measured electric power of each electric power measuring unit 1, 2, 3 is 1000 W (full scale), the output of each electric power measuring unit 1, 2, 3 becomes 1V, respectively.
The voltage Va on the output side of the operational amplifier 4 is obtained by the following equation. Va =-(1VxR4 / R1 + 1VxR4 / R2 + 1VxR4 / R3) =-1V

【0007】したがって、次段の第2オペアンプ5を経
ることで加算電力の出力端子T3には、1Vの出力が得
られることになる。
Therefore, the output of 1V is obtained at the output terminal T3 for the added power by passing through the second operational amplifier 5 in the next stage.

【0008】つまり、3つの電力測定部1,2,3の電
力レンジが同じであれば、加算電力の出力は、1000
W×3をフルスケールとする直流電圧ということにな
る。
That is, if the power ranges of the three power measuring units 1, 2 and 3 are the same, the output of the added power is 1000
This means a DC voltage with W × 3 as the full scale.

【0009】[0009]

【発明が解決しようとする課題】ところで、図2に示す
従来例によれば、簡単な回路構成のもとで、総和の電力
(例えば三相4線ラインの測定を行えば三相4線の総電
力を意味する)に比例した直流電圧が得られる。
By the way, according to the conventional example shown in FIG. 2, the total power (for example, three-phase four-wire is measured if the measurement of the three-phase four-wire line is performed under a simple circuit configuration. A DC voltage proportional to the total power) is obtained.

【0010】しかし、個々の電力測定部1,2,3を用
いて例えば3チャンネルの単相電力を各別に測定する場
合には、それぞれの電力測定部1,2,3に設定される
電力レンジが異なったものとなる結果、第2オペアンプ
5の出力側に位置する加算電力の出力端子T3には、一
応は見かけ上の加算値が得られるものの、設定された電
力レンジとの対応関係が不明なため、実質的に無意味な
データとなってしまう不具合があった。
However, in the case of individually measuring, for example, three-channel single-phase power using the individual power measuring units 1, 2, and 3, the power ranges set in the respective power measuring units 1, 2, and 3 are set. As a result, the apparent added value is obtained at the output terminal T3 of the added power located on the output side of the second operational amplifier 5, but the correspondence with the set power range is unknown. Therefore, there was a problem that the data became virtually meaningless.

【0011】[0011]

【課題を解決するための手段】この発明は、従来技術に
見られた上記課題に鑑みてなされたものであり、その構
成上の特徴は、複数個の電力測定部と、これら電力測定
部からの各出力が直列接続されたそれぞれの抵抗を経て
反転入力端子の側に入力される第1オペアンプと、この
第1オペアンプからの出力が直列接続された抵抗を経て
反転入力端子の側に入力されてその出力を可能に配設さ
れる第2オペアンプとを備え、第1オペアンプと第2オ
ペアンプとのそれぞれは抵抗を有して形成される負帰還
回路が設けられてなる電力測定値の加算回路であって、
電力測定部の各出力側の前記抵抗のそれぞれは、対応す
る電力測定部に設定される電力レンジに反比例してその
抵抗値が選択制御される複数個の切替用抵抗素子を設け
て各別に形成し、第2オペアンプの負帰還回路中の前記
抵抗は、各電力測定部で設定される電力レンジ中、最大
の電力レンジに対応する抵抗値となるように選択制御さ
れる前記切替用抵抗素子と同一構成の切替用抵抗素子を
設けて形成したことにある。
SUMMARY OF THE INVENTION The present invention has been made in view of the above problems found in the prior art. The structural feature of the present invention is that a plurality of power measuring units and these power measuring units are used. Each of the outputs of the first operational amplifier is input to the side of the inverting input terminal through the respective resistances connected in series, and the output from the first operational amplifier is input to the side of the inverting input terminal via the series connected resistance. And a second operational amplifier arranged so that the output thereof can be provided, and a negative feedback circuit formed by each of the first operational amplifier and the second operational amplifier being provided with a negative feedback circuit is provided. And
Each of the resistors on each output side of the power measurement unit is formed separately by providing a plurality of switching resistance elements whose resistance values are selectively controlled in inverse proportion to the power range set in the corresponding power measurement unit. However, the resistance in the negative feedback circuit of the second operational amplifier is the switching resistance element that is selectively controlled so as to have a resistance value corresponding to the maximum power range in the power range set by each power measurement unit. This is because the switching resistance element having the same configuration is provided.

【0012】[0012]

【作用】このため、加算電力の出力端子側には、現在使
用中の電力測定部に設定されている電力レンジのうち、
相対的に最大のレンジをフルスケールとした加算出力が
常に得られることになり、したがって、各電力測定部の
電力レンジの設定状態がどのような組み合わせからなる
ものであっても、正しい加算結果が得られるので、レン
ジ設定の制約をなくすることができる。
Therefore, on the output terminal side of the added power, of the power range set in the power measuring unit currently in use,
Since the addition output with the maximum range relative to the full scale is always obtained, the correct addition result can be obtained regardless of the combination of the setting states of the power ranges of the power measurement units. As a result, the restriction on range setting can be eliminated.

【0013】[0013]

【実施例】以下、図面に基づいてこの発明の実施例を説
明する。
Embodiments of the present invention will be described below with reference to the drawings.

【0014】図1は、この発明の一実施例を示す説明図
であり、その全体は、それぞれが電圧入力端子T1と電
流入力端子T2とを各別に備えてなる3つの電力測定部
11,12,13と、これら電力測定部11,12,1
3からの各出力が直列接続されたそれぞれの抵抗R1,
R2,R3を経て反転入力端子の側に入力される第1オ
ペアンプ14と、この第1オペアンプ14からの出力が
直列接続された抵抗R5を経て反転入力端子の側に入力
され、その出力側に加算電力の出力端子T3を備えてな
る第2オペアンプ15とで構成され、第1オペアンプ1
4には抵抗R4により形成される負帰還回路16が、第
2オペアンプ15には抵抗R6により形成される負帰還
回路17がそれぞれ設けられている。
FIG. 1 is an explanatory view showing an embodiment of the present invention. As a whole, three power measuring units 11 and 12 each having a voltage input terminal T1 and a current input terminal T2 are provided. , 13 and these power measuring units 11, 12, 1
The respective resistors R1 in which the respective outputs from 3 are connected in series
A first operational amplifier 14 that is input to the side of the inverting input terminal via R2 and R3, and an output from this first operational amplifier 14 is input to the side of the inverting input terminal via a resistor R5 that is connected in series, and to the output side thereof. The second operational amplifier 15 is provided with an output terminal T3 for added power, and the first operational amplifier 1
4 is provided with a negative feedback circuit 16 formed by a resistor R4, and the second operational amplifier 15 is provided with a negative feedback circuit 17 formed by a resistor R6.

【0015】この場合、抵抗R1,R2,R3と抵抗R
6とのそれぞれは、いずれも対応するスイッチS1,S
2,S3,S4,S5により開閉制御される切替用抵抗
素子Ra,Rb,Rc,Rd,Reを並列接続すること
で、その抵抗値の切り替えを自在にして形成されてい
る。
In this case, the resistors R1, R2 and R3 and the resistor R
6 and the corresponding switches S1 and S
By connecting in parallel switching resistance elements Ra, Rb, Rc, Rd, Re which are controlled to be opened / closed by 2, S3, S4, S5, the resistance values can be switched freely.

【0016】また、3つの電力測定部11,12,13
は、それぞれが制御部18から制御ライン19を介して
送出されるレンジ制御信号により電力レンジの自動切り
替えが自在となって制御されており、対応する抵抗R
1,R2,R3の抵抗値は、設定される電力レンジの大
きさに反比例する関係のもとで選択的に設定されるよう
になっている。
The three power measuring units 11, 12, 13 are also provided.
Are controlled by a range control signal sent from the control unit 18 via the control line 19 such that the power range can be automatically switched.
The resistance values of 1, R2 and R3 are selectively set in a relationship inversely proportional to the size of the set power range.

【0017】この場合に設定される各電力測定部11,
12,13の電力レンジについては、それぞれが200
0W,1000W,500W,200W,100Wの5
種類の電力レンジを有し、各電力測定部11,12,1
3からの出力V1,V2,V3のそれぞれは電力レンジ
のフルスケールに対し1Vであるとして説明する。
Each power measuring unit 11 set in this case,
Each of the power ranges of 12 and 13 is 200
5 of 0W, 1000W, 500W, 200W, 100W
Each type of power measuring unit 11, 12, 1 has a kind of power range.
Each of the outputs V1, V2 and V3 from 3 will be described as being 1V with respect to the full scale of the power range.

【0018】また、各電力測定部11,12,13に設
定される電力レンジとの対応関係のもとで選択される抵
抗R1,R2,R3の抵抗値、つまり切替用抵抗素子R
a,Rb,Rc,Rd,Reの値については、設定され
る電力レンジに対し表1に示すように反比例する関係の
もとで選ばれ、しかも、R4=1,R5=1とする。な
お、抵抗R6を構成している切替用抵抗素子Ra,R
b,Rc,Rd,Reについても抵抗R1,R2,R3
の場合と同じ対応関係のもとでその抵抗値が設定できる
ものとする。
Further, the resistance values of the resistors R1, R2 and R3 selected in correspondence with the power ranges set in the respective power measuring units 11, 12 and 13, that is, the switching resistance element R.
The values of a, Rb, Rc, Rd, and Re are selected in a relationship that is inversely proportional to the set power range as shown in Table 1, and R4 = 1 and R5 = 1. It should be noted that the switching resistance elements Ra and R that form the resistor R6.
b, Rc, Rd and Re are also resistors R1, R2 and R3
It is assumed that the resistance value can be set under the same correspondence relationship as in the case.

【0019】[0019]

【表1】 [Table 1]

【0020】したがって、電力測定部11,12,13
における各電力レンジについては、チャンネル1として
の電力測定部11が2000W、チャンネル2としての
電力測定部12が500W、チャンネル3としての電力
測定部13が100Wに設定されてフルスケールに相当
する電力を測定しているとすれば、電力測定部11,1
2,13の出力電圧V1,V2,V3のそれぞれはいず
れも1Vということになる。
Therefore, the power measuring units 11, 12, 13
For each power range in, the power measuring unit 11 as the channel 1 is set to 2000 W, the power measuring unit 12 as the channel 2 is set to 500 W, and the power measuring unit 13 as the channel 3 is set to 100 W to set the power corresponding to the full scale. If it is measuring, the power measuring unit 11, 1
Each of the output voltages V1, V2 and V3 of 2 and 13 is 1V.

【0021】つまり、上記設定条件のもとでは、表1に
従い抵抗R1=Ra=1,R2=Rc=4,R3=Re
=20となるように制御部18からレンジ制御信号が出
力されることになる。
That is, under the above setting conditions, the resistors R1 = Ra = 1, R2 = Rc = 4, R3 = Re according to Table 1.
The range control signal is output from the control unit 18 so that = 20.

【0022】かくして、加算電力の出力端子T3の電圧
Voは、Vo=−R6×V4/R5の(1)式により求
められる。
Thus, the voltage Vo at the output terminal T3 of the added power is obtained by the equation (1) of Vo = -R6 * V4 / R5.

【0023】また、図1の回路中、第1オペアンプ14
における出力側の出力電圧V4は、V4=−R4×V1
/R1−R4×V2/R2−R4×V3/R3の(2)
式により求められ、表1に基づきR1には「1」を、R
2には「4」を、R3には「20」の数値をそれぞれ代
入することで、V4=−1.3Vが得られる。
In the circuit of FIG. 1, the first operational amplifier 14
The output voltage V4 on the output side is V4 = −R4 × V1
/ R1-R4 x V2 / R2-R4 x V3 / R3 (2)
Calculated by the formula, based on Table 1, R1 is "1", R
By substituting “4” for 2 and the numerical value of “20” for R3, V4 = −1.3V is obtained.

【0024】他方、抵抗R6については、制御部18か
らの制御信号により3つある電力測定部11,12,1
3のうち、相対的に最大の電力レンジが設定されている
いずれかのものの設定レンジと対応する抵抗値が選択さ
れるように制御されているので、上記設定条件のもとで
は抵抗R6=Ra=1となる。
On the other hand, regarding the resistor R6, there are three power measuring units 11, 12, 1 according to the control signal from the control unit 18.
Among the three, the resistance value corresponding to the setting range of any one in which the relatively maximum power range is set is controlled so that the resistance R6 = Ra under the above setting conditions. = 1.

【0025】しかして、前記(1)式であるVo=−R
6×V4/R5にR6=R5=1とV4=−1.3Vと
を代入することで、加算電力の出力端子T3の電圧Vo
=1.3Vが得られることになる。
Then, Vo = -R which is the above-mentioned formula (1).
By substituting R6 = R5 = 1 and V4 = −1.3V into 6 × V4 / R5, the voltage Vo at the output terminal T3 of the added power is obtained.
= 1.3V will be obtained.

【0026】ここで、設定されている電力レンジ200
0W(フルスケール)に対し加算電力の出力端子T3の
電圧Voが1Vであることを考慮すると、Voが1.3
Vである場合は、電力として2600Wに相当し、3つ
の電力測定部11,12,13によって測定した電力の
総和(2000W+500W+100W)に等しいこと
になる。
Here, the set power range 200
Considering that the voltage Vo at the output terminal T3 of the added power is 1 V with respect to 0 W (full scale), Vo is 1.3.
In the case of V, the electric power corresponds to 2600 W, which is equal to the total power (2000 W + 500 W + 100 W) measured by the three power measuring units 11, 12, and 13.

【0027】この発明は上述したようにして構成されて
いるので、電力測定部11,12,13からの出力電圧
V1,V2,V3のそれぞれは、いずれも1Vで出力さ
れることになり、対応する抵抗R1,R2,R3のそれ
ぞれでは、切替用抵抗素子Ra,Rb,Rc,Rd,R
eのうちから電力測定部11,12,13に設定されて
いる電力レンジに反比例する抵抗値が得られるようにス
イッチS1,S2,S3,S4,S5が制御部18から
の制御信号に基づいて開閉制御され、有効になる切替用
抵抗素子が選択される。
Since the present invention is configured as described above, each of the output voltages V1, V2, V3 from the power measuring units 11, 12, 13 will be output at 1V. The switching resistance elements Ra, Rb, Rc, Rd, and R are provided in the respective resistors R1, R2, and R3.
Based on the control signal from the control unit 18, the switches S1, S2, S3, S4, S5 are provided so that a resistance value inversely proportional to the power range set in the power measurement units 11, 12, 13 is obtained from e. The switching resistance element that is controlled to be opened and closed and becomes effective is selected.

【0028】このため、加算電力の出力端子T3側に
は、現在使用中の電力測定部11,12,13に設定さ
れている電力レンジのうち、相対的に最大のレンジをフ
ルスケールとした加算出力が常に得られることになる。
Therefore, on the side of the output terminal T3 for the added power, the addition of the maximum range of the power ranges currently set in the power measuring units 11, 12, and 13 as the full scale is added. The output will always be available.

【0029】したがって、各電力測定部11,12,1
3の電力レンジの設定状態がどのような組み合わせから
なるものであっても、正しい加算結果が得られるので、
各電力測定部11,12,13のそれぞれの電力レンジ
を等しくしなければならないというようなレンジ設定上
の制約をなくすることができる。
Therefore, each power measuring unit 11, 12, 1
Since the correct addition result can be obtained regardless of the combination of the setting states of the power range of No. 3,
It is possible to eliminate the restriction on the range setting such that the respective power ranges of the power measuring units 11, 12, and 13 must be equal.

【0030】[0030]

【発明の効果】以上述べたようにこの発明によれば、加
算電力の出力端子側には、現在使用中の電力測定部に設
定されている電力レンジのうち、相対的に最大のレンジ
をフルスケールとした加算出力が常に得られることにな
り、したがって、各電力測定部の電力レンジの設定状態
がどのような組み合わせからなるものであっても、正し
い加算結果が得られるので、レンジ設定上の制約をなく
することができる。
As described above, according to the present invention, on the output terminal side of the added power, a relatively maximum range among the power ranges set in the power measuring unit currently in use is full. The scaled addition output is always obtained. Therefore, the correct addition result can be obtained regardless of the combination of the setting states of the power ranges of the power measurement units. The constraint can be removed.

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

【図1】この発明の一実施例を示す回路説明図。FIG. 1 is an explanatory circuit diagram showing an embodiment of the present invention.

【図2】従来例についての電力測定値の加算回路説明
図。
FIG. 2 is an explanatory diagram of a power measurement value addition circuit for a conventional example.

【符号の説明】[Explanation of symbols]

11 電力測定部 12 電力測定部 13 電力測定部 14 第1オペアンプ 15 第2オペアンプ 16 負帰還回路 17 負帰還回路 18 制御部 19 制御ライン T1 電圧入力端子 T2 電流入力端子 T3 加算電力出力端子 S1 スイッチ S2 スイッチ S3 スイッチ S4 スイッチ S5 スイッチ Ra 切替用抵抗素子 Rb 切替用抵抗素子 Rc 切替用抵抗素子 Rd 切替用抵抗素子 Re 切替用抵抗素子 Reference Signs List 11 power measuring unit 12 power measuring unit 13 power measuring unit 14 first operational amplifier 15 second operational amplifier 16 negative feedback circuit 17 negative feedback circuit 18 control unit 19 control line T1 voltage input terminal T2 current input terminal T3 added power output terminal S1 switch S2 Switch S3 switch S4 switch S5 switch Ra switching resistor element Rb switching resistor element Rc switching resistor element Rd switching resistor element Re switching resistor element

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 複数個の電力測定部と、これら電力測定
部からの各出力が直列接続されたそれぞれの抵抗を経て
反転入力端子の側に入力される第1オペアンプと、この
第1オペアンプからの出力が直列接続された抵抗を経て
反転入力端子の側に入力されてその出力を可能に配設さ
れる第2オペアンプとを備え、第1オペアンプと第2オ
ペアンプとのそれぞれは抵抗を有して形成される負帰還
回路が設けられてなる電力測定値の加算回路において、
電力測定部の各出力側の前記抵抗のそれぞれは、対応す
る電力測定部に設定される電力レンジに反比例してその
抵抗値が選択制御される複数個の切替用抵抗素子を設け
て各別に形成し、第2オペアンプの負帰還回路中の前記
抵抗は、各電力測定部で設定される電力レンジ中、最大
の電力レンジに対応する抵抗値となるように選択制御さ
れる前記切替用抵抗素子と同一構成の切替用抵抗素子を
設けて形成したことを特徴とする電力測定値の加算回
路。
1. A plurality of power measuring units, a first operational amplifier in which outputs from the power measuring units are input to the inverting input terminal side via respective resistors connected in series, and the first operational amplifier. A second operational amplifier arranged so that its output can be output by being input to the inverting input terminal side through a resistor connected in series, and each of the first operational amplifier and the second operational amplifier has a resistor. In the addition circuit of the measured power value, which is provided with a negative feedback circuit formed by
Each of the resistors on each output side of the power measurement unit is formed separately by providing a plurality of switching resistance elements whose resistance values are selectively controlled in inverse proportion to the power range set in the corresponding power measurement unit. However, the resistance in the negative feedback circuit of the second operational amplifier is the switching resistance element that is selectively controlled so as to have a resistance value corresponding to the maximum power range in the power range set by each power measurement unit. An addition circuit of measured power values, which is formed by providing switching resistance elements having the same configuration.
JP22207092A 1992-07-29 1992-07-29 Power measurement value addition circuit Expired - Fee Related JP3199284B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22207092A JP3199284B2 (en) 1992-07-29 1992-07-29 Power measurement value addition circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22207092A JP3199284B2 (en) 1992-07-29 1992-07-29 Power measurement value addition circuit

Publications (2)

Publication Number Publication Date
JPH0651002A true JPH0651002A (en) 1994-02-25
JP3199284B2 JP3199284B2 (en) 2001-08-13

Family

ID=16776649

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22207092A Expired - Fee Related JP3199284B2 (en) 1992-07-29 1992-07-29 Power measurement value addition circuit

Country Status (1)

Country Link
JP (1) JP3199284B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010153967A (en) * 2008-12-24 2010-07-08 Kyocera Corp Addition circuit, power amplifying circuit using the addition circuit, transmitter using the power amplifying circuit, and communication device
JP2016061642A (en) * 2014-09-17 2016-04-25 日置電機株式会社 Measurement device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010153967A (en) * 2008-12-24 2010-07-08 Kyocera Corp Addition circuit, power amplifying circuit using the addition circuit, transmitter using the power amplifying circuit, and communication device
US8351881B2 (en) 2008-12-24 2013-01-08 Kyocera Corporation Addition circuit, power amplifier circuit using same, and transmission device and communication device using the power amplifier circuit
JP2016061642A (en) * 2014-09-17 2016-04-25 日置電機株式会社 Measurement device

Also Published As

Publication number Publication date
JP3199284B2 (en) 2001-08-13

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