Entropy change in an RC circuit

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Homework Help Overview

The discussion revolves around the entropy change in an RC circuit involving a cylindrical capacitor charged isothermally. The original poster presents a scenario where the capacitor is discharged and then charged while interacting with a thermal reservoir, raising questions about the entropy of the universe and the dependencies of certain coefficients in the context of thermodynamics.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the physical picture of the capacitor in a thermal reservoir and question the implications of charging the capacitor isothermally. There are inquiries about the expression for the entropy change and the role of heat in the RC circuit analysis.

Discussion Status

Some participants have offered insights into the thermodynamic principles at play, discussing the relationship between work, heat, and entropy. There is a recognition of the complexities involved in analyzing the system, particularly regarding the assumptions about reversibility and the nature of the processes occurring within the circuit.

Contextual Notes

There are indications of confusion regarding the treatment of heat in RC circuits, as well as the behavior of capacitance with temperature. The discussion also touches on the irreversible nature of current flow through resistors and the associated entropy changes.

yamata1
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Hello,I would like some help for a problem

Homework Statement


Initially:At t=0 [/B]the cylindrical capacitor of capacitance c=\frac{\epsilon s}{d} (d the distance between the 2 electrodes and s their surface; \epsilon = \epsilon(T) is the dielectric permittivity) is discharged and we close the circuit and charge isothermally the cylindrical capacitor until it has a c*v charge.
The current is i=\frac{dq}{dt} and the voltage is v(t), the electric charge of the capacitor is q(t)=c*v(t).
We have an RC circuit receiving work W from a generator of voltage v and energy Q_{exchanged} from a thermal reservoir (thermostat) of T_0 Kelvin,the circuit has its entropy change\Delta S_{in} during the charging.
We have C_q the heat capacity for a constant charge q and \lambda= \frac{qT \epsilon'}{\epsilon c} another coefficient in the equation :
TdS_{in}= C_q dT + \lambda dq (1)

What is the entropy of the universe \Delta S_{univ} equal to ?
Does C_q depend on q ?

Homework Equations


\Delta S_{thermostat}=\frac{Q_{exchanged}}{T_0}

The Attempt at a Solution


If we integrate C_q over T ,I think q does appear in the formula for C_q but it's not a variable I think.To find \Delta S_{in} we divide the equation (1) by T then integrate \frac{\lambda}{T} over q from 0 to q=cv.
\Delta S_{univ}=\Delta S_{thermostat}+\Delta S_{in}
I would like to know how to express \Delta S_{thermostat} and it's sign. Thank you.
 
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What physical physical picture you are trying to work with? That is, what phenomenon are you interested in? It seems you have the capacitor bathed in a temperature reservoir. Why?
 
Gene Naden said:
What physical physical picture you are trying to work with? That is, what phenomenon are you interested in? It seems you have the capacitor bathed in a temperature reservoir. Why?

I want to know how to express the entropy change , I think the entropy change of the universe is 0 but I'm not sure what the equation is.The RC circuit is getting heat from the reservoir and work from the generator,I'm guessing it's to make it a reversible process.
 
I am not sure, but I suspect you are confused. Ordinarily one does not consider heat when analyzing an RC circuit, and the capacitance of a capacitor does not vary much with temperature. I am not so sure that the net change in entropy of the universe is zero; For irreversible processes, entropy increases.

Generally the flow of current through a circuit with resistance is not a reversible process. The resistors give off heat but never absorb heat.
 
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This is pretty advanced thermodynamics. I can only give you some ideas:
Since the capacitor is being charged isothermally, dT = 0 and you are left with dS = \lambda dq/T = (ε'/εc)q dq. You didn't say what ε' and c are. But your eq. (1) is of course a form of the Maxwell "2nd T dS equation" so there must exist a coefficient representing the change of polarization with T ( related by the state equation). So maybe ε' = dε/dT and ΔSdielectric = (ε'/εc) ∫q dq from q=0 to q = Cv.
Then the total change in entropy of the universe is just ΔSdielectric - ΔSthermostat.

Sorry, not very definite; hope others will do better.
 
I think I have an explanation :

The generator gives the system {resitance,capacitor} the electric energy :

ile_TEX.cgi?q_{f}.e=c.gif


The capacitor charges itself by en absorbing half ( the work ##W=\int vdq##). The difference represents the lost energy through the Joule effect :

ile_TEX.cgi?E_{Joule}=\frac{1}{2}q_{f}.e=\frac{1}{2}c.gif


This energy is received through heat by the heat reservoir at fixed temperature ,which increases the entropy by :
ile_TEX.cgi?\frac{q_{f}^{2}}{2c.gif


Accouting for the resistance, we have :
\Delta S_{univ}=\frac{\varepsilon'}{2\varepsilon.c}\cdot q_{f}^{2}-\frac{\varepsilon'}{2\varepsilon.c}\cdot q_{f}^{2}+\frac{q_{f}^{2}}{2c.T_{0}}=\frac{q_{f}^{2}}{2c.T_{0}}

there is a creation of entropy caused by the Joulet effect which is an irreversible phenomenon as Gene Naden wrote
Gene Naden said:
I am not sure, but I suspect you are confused. Ordinarily one does not consider heat when analyzing an RC circuit, and the capacitance of a capacitor does not vary much with temperature. I am not so sure that the net change in entropy of the universe is zero; For irreversible processes, entropy increases.

Generally the flow of current through a circuit with resistance is not a reversible process. The resistors give off heat but never absorb heat.
.
The power received by the heat reservoir is the power produced by the Joule effect :

ile_TEX.cgi?P_{Joule}=r.i^{2}=r.gif


ile_TEX.cgi?\frac{dS_{univ}}{dt}=\frac{P_{Joule}}{T_{0}}=\frac{r}{T_{0}}.gif
 

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  • ile_TEX.cgi?E_{Joule}=\frac{1}{2}q_{f}.e=\frac{1}{2}c.gif
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  • ile_TEX.cgi?\frac{q_{f}^{2}}{2c.gif
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  • ile_TEX.cgi?P_{Joule}=r.i^{2}=r.gif
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  • ile_TEX.cgi?\frac{dS_{univ}}{dt}=\frac{P_{Joule}}{T_{0}}=\frac{r}{T_{0}}.gif
    ile_TEX.cgi?\frac{dS_{univ}}{dt}=\frac{P_{Joule}}{T_{0}}=\frac{r}{T_{0}}.gif
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