What is the Voltage on C1/C2 after the switch closes?

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Discussion Overview

The discussion revolves around the behavior of two capacitors in an RC circuit after a switch is closed. Participants explore the equations relevant to determining the voltage across the capacitors over time, the concept of time constant (Tau), and the conservation of charge in the circuit. The scope includes theoretical considerations, mathematical reasoning, and conceptual clarifications related to capacitor behavior in series.

Discussion Character

  • Homework-related
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant suggests using the equation Vf + (Vi - Vf)e^(-t/RC) to find voltage in an RC circuit, questioning its applicability due to the presence of a second capacitor.
  • Another participant argues that the relevant equation applies to charging from a constant voltage and questions the context of the question, noting that voltage is time-dependent.
  • Some participants propose that total charge is conserved and that the potentials across the two capacitors must be equal at steady state.
  • There is a discussion about whether the time scale for plotting voltage can be logarithmic to reveal exponential changes.
  • One participant mentions that the eventual voltage state is 0.6V, while another clarifies that charge is not the same as voltage and discusses the relationship between charge and voltage for capacitors.
  • Concerns are raised about the proper way to sum capacitances in series versus parallel, with some participants providing calculations for total capacitance and charge distribution.
  • There is a correction regarding the use of units, specifically the distinction between femtoFarads and Farads, as well as the difference between energy and potential difference.

Areas of Agreement / Disagreement

Participants express differing views on the appropriate equations to use and the implications of capacitor behavior in the circuit. There is no consensus on a single approach or solution, and multiple competing views remain regarding the interpretation of the circuit's behavior and the relevant calculations.

Contextual Notes

Participants note limitations in understanding the context of the question, including the time-dependent nature of voltage and the need for clarification on the equations to use. There are unresolved discussions about the correct approach to calculating Tau and the implications of charge conservation in the circuit.

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Homework Statement


upload_2018-11-17_20-30-10.png


Homework Equations



Vf+(Vi-Vf)e-t/RC

Tau = RC

The Attempt at a Solution


upload_2018-11-17_20-20-48.png
[/B]

Normally, I would use the eq'n mentioned above to find Vr in an RC circuit. However, this second capacitor is throwing me off. Is there a new equation I should use? How do I think about this circuit?
Additionally, how would I go about finding Tau? Do I add the capacitance of each capacitor:
(R x (C1+C2))?

Thanks.
 

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Hi,

Your relevant equation applies to charging from a constant voltage, so not in this case. You need something better.

The context of the question is unclear to me: there is no single 'the voltage after the switch closes': as your plot clearly shows, Vr is time dependent. From the remainder of the exercise it seems they mean 'after a long time'. But you are using some simulation programme to plot the time dependence (which as said is not described by your relevant equation).
 
Are you able to set the time scale to be logarithmic for that plot? If the rate of voltage change reveals as a straight line on semilog axes then you can say the voltage is changing exponentially with time.

But all the question seems to require is that you allow the system sufficient time to settle at its new equilibrium, and determine a value for this final steady state voltage.
 
Hint: Total charge is conserved and the potentials across the two capacitors must be equal when the circuit reaches steady state.
Lapse said:
Additionally, how would I go about finding Tau? Do I add the capacitance of each capacitor:
(R x (C1+C2))?
The capacitors and resistance (of the switch) are all in series.
 
BvU said:
Hi,

Your relevant equation applies to charging from a constant voltage, so not in this case. You need something better.

The context of the question is unclear to me: there is no single 'the voltage after the switch closes': as your plot clearly shows, Vr is time dependent. From the remainder of the exercise it seems they mean 'after a long time'. But you are using some simulation programme to plot the time dependence (which as said is not described by your relevant equation).

I understand. So what would the relevant equation be?
 
gneill said:
Hint: Total charge is conserved and the potentials across the two capacitors must be equal when the circuit reaches steady state.

The capacitors and resistance (of the switch) are all in series.

I noticed that both capacitor charges become equal (they converge to 0.6V).

I see that they are in series; however, what does this mean for finding Tau?
 
NascentOxygen said:
Are you able to set the time scale to be logarithmic for that plot? If the rate of voltage change reveals as a straight line on semilog axes then you can say the voltage is changing exponentially with time.

But all the question seems to require is that you allow the system sufficient time to settle at its new equilibrium, and determine a value for this final steady state voltage.

The graph being set at a time stop of 200ps was set by the professor. This is why I am assuming that instead of showing a final state at 0.6V, he probably wants to see an equation for the voltage over each capacitor proving what the voltage would be if the time stop went beyond 200ps.
What is a relevant equation I can use to solve for the voltages over the capacitors?
 
Lapse said:
I noticed that both capacitor charges become equal (they converge to 0.6V).
No. Charge is not voltage (look at the units). What's the relationship between charge and voltage for a capacitor?

The capacitors will not have equal charges for the same potential difference as they do not have the same capacitance.
I see that they are in series; however, what does this mean for finding Tau?
Well for one thing the capacitors are in series... What's the net capacitance?

Note that you don't need ##\tau## to answer this question. You only need to find the eventual state of the system (voltages, charges).

Charge is conserved. After a long time the potential differences across the capacitors must be equal. So how will the (conserved) charge be distributed?
 
gneill said:
No. Charge is not voltage (look at the units). What's the relationship between charge and voltage for a capacitor?
Q = C x V
gneill said:
Well for one thing the capacitors are in series... What's the net capacitance?
C1 + C2 = 50f + 200f = 250f
gneill said:
Note that you don't need ττ\tau to answer this question. You only need to find the eventual state of the system (voltages, charges).
The eventual voltage state is 0.6V.
The eventual charge state, hmm...
Q1 = 50f x 0.6V = 30 coulombs
Q2 = 200f x 0.6V = 120 coulombs
gneill said:
Charge is conserved. After a long time the potential differences across the capacitors must be equal. So how will the (conserved) charge be distributed?
Once the capacitors are fully charged they behave like wires, correct? It would then make sense that what follows is an equal potential difference (this would be similar to how a current is equal on either end of a closed loop, correct?).
Q = C x V = 250f x 0.6V = 150 coulombs
 
  • #10
Ahh, tell me if I'm thinking of it correctly now!

The energy after the switch closes:
E1 = 9J
E2 = 36J

But before the switch closes:
E1 = 25J
E2 = 50J

After potential difference: 36J - 9J = 25J
Before potention difference: 50J - 25J = 25J

25J = 25J ...gneill, is this what you meant by:
gneill said:
After a long time the potential differences across the capacitors must be equal.
 
  • #11
Lapse said:
Once the capacitors are fully charged they behave like wires, correct
No !
(Ideal) wires have ##\Delta V=0\ \ \forall I \ ##
(Ideal) capacitors have ##Q = CV \Rightarrow I = C{dV\over dt}## which is something completely different !

images?q=tbn:ANd9GcRkP_HZS3y1bNfbC5dg9786Bz0f7-nLLZkauCf3UbvaN1Y_uGrh.jpg
 

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  • #12
Lapse said:
C1 + C2 = 50f + 200f = 250f
That is how to add capacitors in parallel. How do capacitors in series sum?
Lapse said:
The eventual voltage state is 0.6V.
The eventual charge state, hmm...
Q1 = 50f x 0.6V = 30 coulombs
Q2 = 200f x 0.6V = 120 coulombs
Small "f" is not Farads (capital "F"). Small f designates the femto prefix (10-15).
Lapse said:
Ahh, tell me if I'm thinking of it correctly now!

The energy after the switch closes:
E1 = 9J
E2 = 36J

But before the switch closes:
E1 = 25J
E2 = 50J
You'll need to redo the above taking into account that the capacitor values are given in femtoFarads. Also, check your math for the "before the switch closes" value for E2.
After potential difference: 36J - 9J = 25J
Before potention difference: 50J - 25J = 25J
Energy is not potential. Potential difference is measured in Volts.
 
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