Entropy change in an RC circuit

AI Thread Summary
The discussion focuses on the entropy change in an RC circuit during the isothermal charging of a cylindrical capacitor. The participants analyze the relationship between the heat capacity at constant charge and the charge itself, questioning whether the heat capacity depends on the charge. They explore the total entropy change of the universe, emphasizing that the process is irreversible due to the Joule effect, which contributes to increased entropy. The conversation highlights the complexities of integrating thermodynamic principles with electrical circuit behavior, particularly regarding the interplay of work, heat exchange, and entropy. Overall, the consensus suggests that the net change in entropy of the universe is not zero, reflecting the irreversible nature of the process.
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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