Opamp adder circuit: Where does the "-" come from?

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Discussion Overview

The discussion revolves around the analysis of an operational amplifier (op-amp) adder circuit, specifically focusing on the origin of the negative sign in the output voltage equation. Participants explore the application of Kirchhoff's Current Law (KCL) in this context, addressing current flow and polarity at a node in the circuit.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express confusion about the negative sign in the output voltage equation, questioning its origin and the direction of current flow from the resistor R3.
  • One participant suggests that when the input voltage increases, the output of the op-amp must decrease to maintain the virtual ground at the negative input.
  • Another participant emphasizes the importance of consistent polarity when applying KCL, noting that all currents flowing into a node should sum to zero.
  • There is a discussion about whether the sum of currents flowing into the node equals the sum of currents flowing out, with some participants asserting that the currents should flow to R3.
  • One participant clarifies that if currents are defined as flowing into the node, any current flowing out must be assigned a negative sign in the KCL equation.
  • Several participants agree on the utility of consistently writing KCL equations with all current arrows pointing into the node to avoid sign errors.
  • Concerns are raised about the complexity of defining all currents in more complicated networks, with a note on the potential for errors in both KCL and Kirchhoff's Voltage Law (KVL) applications.

Areas of Agreement / Disagreement

Participants generally agree on the need for consistent polarity in KCL equations, but there remains some disagreement about the interpretation of current flow and the implications of the negative sign in the output equation.

Contextual Notes

Participants highlight the importance of carefully accounting for current polarities and the potential for errors in circuit analysis, particularly in more complex networks.

altruan23
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Homework Statement
I was analyzing the adder circuit and I dont understand from where does the - come in the Vout equation.
Relevant Equations
KCL
So i used KCL and both currents are flowing into the node, and then leaving together to go to the resistor R3.
So my eq can be seen in the picture. I was looking in a book and they had a minus infront of the parantheses.
Is the current flowing from R3 into the node??
1647963385469.png
 
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altruan23 said:
Homework Statement:: I was analyzing the adder circuit and I don't understand from where does the - come in the Vout equation.
Relevant Equations:: KCL

So i used KCL and both currents are flowing into the node, and then leaving together to go to the resistor R3.
So my eq can be seen in the picture. I was looking in a book and they had a minus infront of the parantheses.
Is the current flowing from R3 into the node??
View attachment 298767
I'm not able to read your image (in the future, please type your work into the forum using LaTeX -- see the LaTeX Guide link below the Edit window).

But intuitively, when the input voltage goes positive, the output of the opamp needs to go negative to keep it's "-" input at ground (using the "virtual ground" property of an opamp with its "+" input at ground). Does that make any sense to you?
 
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When you make an equation from KCL at a node, you must be careful to be consistent with the polarities of the currents. Try again with the following rule: All currents flowing into a circuit node sum to zero.
 
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isnt it that the sum of the currents flowing into the node, is the same as the sum of the currents flowing out of the node. and schouldnt the sum of both currents flow to the R3?
 
so that means i1+i2= i3 and that is what my KCL is saying.
i set i3 as leaving the node, because there's a virtual ground so it needs to go to R3.
 
altruan23 said:
isnt it that the sum of the currents flowing into the node, is the same as the sum of the currents flowing out of the node. and schouldnt the sum of both currents flow to the R3?
Yes, you can use "into" or "out of". But your equation has some polarities as into and others out of. You must choose one version and remain consistent.

So, that "- node" is at zero volts, which we could name ## V_{neg} \equiv 0 ## (the ideal op-amp with negative feedback assumption). So, the current flowing into the that node from ##V_1 ##, ## I_1 \equiv \frac{(V_1 - V_{neg})}{R1} = \frac{(V_1)}{R1} ##. Same for all of the other currents into the that node ##I_n \equiv \frac{(V_n - V_{neg})}{Rn} = \frac{(V_n)}{Rn} ##.

If you choose the "into" rule than any current polarity that is flowing "out of" the node (as you've defined by your arrows) has to have a - sign added to correct the polarity.

Yes, the sum of ## I_1 + I_2 = I_3 ## given the polarities you've defined. This is equivalent to ## I_1 + I_2 - I_3 = 0 ## which is KCL at the ##V_{neg}## node. ## I_1 ## and ## I_2 ## flow into the node, ## I_3 ## flows out of the node, so it gets a - sign in KCL. Also, ## I_3 \equiv \frac{(V_{neg} - V_o )}{R3} = \frac{(-V_o)}{R3} ##, again with your polarity choice.
 
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altruan23 said:
so that means i1+i2= i3
I still prefer to write it as I1 + I2 + I3 = 0 with all of the current arrows pointing into the node. That helps me to avoid making brain-fade type of mistakes.
 
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berkeman said:
I still prefer to write it as I1 + I2 + I3 = 0 with all of the current arrows pointing into the node. That helps me to avoid making brain-fade type of mistakes.
Me too. The problem with sign errors is that it's conceptually easy to understand, but really easy to slip up and actually do it wrong. It is really helpful to just have a rule that you always try to follow. With experience, we learn that these mistakes are easier to avoid than to find and correct.
 
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Also, in more complicated networks it is often impossible to define all of the currents flowing into nodes. Sometimes current flows out of one node and then into another. So, you just have to be really careful at the beginning to properly account for the polarities when you make the equations. There's an identical problem with KVL, adding voltages in loops.
 
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