Entropy change in an RC circuit

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SUMMARY

The discussion focuses on the entropy change in an RC circuit during the isothermal charging of a cylindrical capacitor. The capacitor, characterized by capacitance \( c = \frac{\epsilon s}{d} \), is charged with a voltage \( v \) while receiving work \( W \) from a generator and energy \( Q_{exchanged} \) from a thermal reservoir at temperature \( T_0 \). The entropy change of the universe \( \Delta S_{univ} \) is expressed as \( \Delta S_{univ} = \Delta S_{thermostat} + \Delta S_{in} \), where \( \Delta S_{thermostat} = \frac{Q_{exchanged}}{T_0} \). The discussion concludes that the net change in entropy is not zero due to the irreversible nature of the Joule effect in resistive circuits.

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  • Familiarity with thermodynamic principles, particularly entropy
  • Knowledge of dielectric materials and their properties
  • Basic calculus for integrating thermodynamic equations
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  • Study the Maxwell relations in thermodynamics
  • Learn about the Joule effect and its implications in electrical circuits
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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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