Electric Circuit Capacitor Charge question

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Discussion Overview

The discussion revolves around the analysis of an RC circuit containing two capacitors and a resistor, focusing on determining the functions governing current and voltage across the capacitors. Participants explore the implications of initial conditions and the application of Kirchhoff's voltage law (KVL) in the context of the circuit's behavior over time.

Discussion Character

  • Homework-related
  • Mathematical reasoning
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant describes the circuit configuration and the initial conditions for the capacitors, expressing confusion over the resulting equations for charge and current.
  • Another participant suggests that the initially charged capacitor should act as a voltage source and discharge exponentially, questioning the initial reasoning.
  • A request for clarification on the terms "reverse polarity" and "regular polarity" is made, indicating a need for visual representation.
  • One participant challenges the complexity of the original poster's approach, suggesting a simpler method by focusing on loop current rather than charge.
  • Another participant provides a loop equation involving integrals of current, prompting further discussion on its validity and the role of the initial voltage in the circuit.
  • There is a back-and-forth regarding the presence of the 40V term in the loop equation, with some participants asserting its relevance as an initial condition.

Areas of Agreement / Disagreement

Participants express differing views on the approach to solving the problem, with some advocating for a focus on current and others emphasizing charge. There is no consensus on the correct method or the interpretation of initial conditions.

Contextual Notes

Participants note potential confusion regarding the initial conditions and the interpretation of voltage sources in the circuit. The discussion reflects varying levels of understanding of circuit analysis techniques and the implications of initial capacitor states.

Who May Find This Useful

This discussion may be useful for students and practitioners interested in circuit analysis, particularly those grappling with the application of KVL in RC circuits and the implications of initial conditions on circuit behavior.

cmmcnamara
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Homework Statement



An RC circuit is given with a 1μF capacitor, a 25kΩ resistor and a 4μF capacitor, all in series. Initially, the 1μF capacitor has a voltage of 40V, while the 4μF capacitor has a voltage of 0V. The circuit, starting from the left and going clockwise is, 1μF (reverse polarity), the resistor and then the 4μF capacitor (regular polarity).

The goal is to find the functions governing current and the voltage of each capacitor (total of three functions).

i(t)=?, v1(t)=?, v4(t)=?


Homework Equations



\sumV=0
V=IR
Q=CV
I=dQ/dt

The Attempt at a Solution



Applying KVL I get:

V1=Vr+V4

Q1/C1=IR+Q2/C2

Q1/C1=Q'R+Q2/C2

This equation becomes very confusing to me. Firstly there are two charge functions of time. I can eliminate this problem by noting that since the circuit is a series, the current is constant throughout all elements meaning that dQ1/dt=dQ2/dt, so I can differentiate this DE and get:

Q1'/C1=Q1''R+Q1'/C2

Q1''+[(C1-C2)/(C1C2R)]Q1'=0

Which leads me to conclude that:

Q1(t)= k1+k2exp([(C2-C1)/(C1C2R)]t

however I can go further, because since I=dQ1/dt=dQ2/dt, then Q2=∫(dQ1/dt)dt, so I get the following:

Q1(t)= k1+k2exp([(C2-C1)/(C1C2R)]t
Q2(t)= k3+k2exp([(C2-C1)/(C1C2R)]t
I(t)= ([(C2-C1)/(C1C2R)]k2exp([(C2-C1)/(C1C2R)]t

However, this leads to a problem. The initial conditions are:

Q1(0)=C1V1i=(1μF)(40V)=40μC
Q2(0)=C2V2i=(4μF)(0V)=0μC
I(0)=0 A

Which gives me:

k1=40 μC
k2=0 μC
k3=0 μC

and:

Q1(t)= 40 μC
Q2(t)= 0 μC
I(t)= 0 A

Can someone point out the error in my reasoning? I've been over it countless times and it all makes sense to me, but there is obviously a problem.
 
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Am at work right now so will try this problem later on. But on first glance...when the circuit is made, then given that the initial voltage on the 1uf cap is 40V, it should act as a voltage source of V=40V at t=0, and then exponentially discharge, no?
 
What do you mean by "reverse polarity" and "regular polarity"? A sketch showing polarity definition would help.
 
cmmcnamara,

Can someone point out the error in my reasoning? I've been over it countless times and it all makes sense to me, but there is obviously a problem.

I did not even bother to look at your work, because I can tell right away that you are making too big a deal out of it. It is a simple single loop equation. Set up the differential loop equations for the two caps and the resistor and solve. Forget about charge and just solve for the loop current. That's all there is to it. So set up the equations and I will let you know if you did it correctly. Then you can continue on to solve the equation for current.

Ratch
 
That is how I derived the differential equation for charge, I used KVL around the loop and applied the information for the caps and resistor. If I find the function for charge the voltage function for each capacitor will be easy to determine using their capacitance and the derivative of the charge function will be the current through the loop because all elements are in series. I think the problem may lie in my choice of initial conditions but I don't see it.
 
cmmcnamara,

Here is the loop equation. Remember V=(1/C)∫i(t)dt

(1/C1)∫i(t)dt+(1/C2)∫i(t)dt+i(t)*R+40=0

Can you solve this differential equation?

Ratch
 
I'm not I understand your loop equation. There is no voltage source in the loop, so I'm not understanding where the 40V term is coming from.
 
cmmcnamara,

There is no voltage source in the loop, so I'm not understanding where the 40V term is coming from.


Sure there is. One of the caps is energized to 40 volts, isn't it?

Ratch
 
Yes initially it is so wouldn't that be part of the initial conditions?
 
  • #10
cmmcnamara,

Yes initially it is so wouldn't that be part of the initial conditions?

Yes, it is. Mathematically, a constant voltage source in series with a unenergized cap is the same as a cap energized at the same voltage with no voltage source in series.

Ratch
 

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