Heat in a resistor (circuit with inductor and capacitor)

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Homework Help Overview

The problem involves a circuit with a voltage source, capacitor, inductor, and resistors, focusing on the heat dissipation in the resistor after a switch is opened. The context includes concepts from circuit theory, particularly involving energy storage and dissipation in reactive components.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the implications of opening the switch after a long time, leading to LC oscillations and energy dissipation. There are attempts to derive equations for energy and heat loss, with some questioning the behavior of current in the inductor post-switch opening.

Discussion Status

Participants are exploring various interpretations of the problem, particularly regarding the initial energy of the system and the relationship between heat loss in different resistors. Some guidance has been offered regarding the calculation of initial energy and the behavior of current in the circuit.

Contextual Notes

There is some confusion regarding the specifics of the switch and its role in the circuit, as well as the assumptions made about the state of the circuit components when the switch is opened.

Rugile
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Homework Statement


A source of ε = 10V, capacitor of C = 5 μf, inductor of L = 15 mH and r = 10 Ω and a resistor of R = 100 Ω are connected as in the schematic (attached). How much heat will dissipate in the resistor after the switch is opened?


Homework Equations



dQ = I2Rdt
KVL

The Attempt at a Solution



First of all I was quite confused by the question, so I just assumed that the switch is opened after a long time, when the capacitor and the inductor are fully charged. Then the voltage across the capacitor is U0 = ε and the current in the inductor is I0 = ε / (R+r). We can write the equation (KVL):
[itex]L\frac{dI}{dt} + I(R+r) + U_C = 0[/itex], where UC is the voltage across the capacitor. I get stuck here - I suppose I could write second order differential equation involving the function of q: [itex]L \frac{d^2 q}{dt^2} + (R+r) \frac{dq}{dt} + \frac{C}{q} = 0[/itex], but I'm not sure what to do with that either. Any hints?
 

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Step 1: After switch is opened, LC oscillation occurs as described by your equation.
Step 2: Heat loss through R and r. Your task is to find out the heat loss thorugh R. At the end, all energy is dissipated through heat loss. So I suggest you find the ratio between heat loss through R: heat loss through r. I also suggest you find the initial energy.
Step 3: The ratio can be found from the ratio of R:r.
 
Okay, so it is enough to find the initial energy of the system and then calculate the heat loss in R using the ratio? Can I say that the initial energy of the system (after opening the switch) was [itex]E = \frac{CU^2}{2} + \frac{LI^2}{2}[/itex], where [itex]I = \frac{\epsilon}{R+r}[/itex] and U = epsilon = EMF ?
 
rude man said:
What switch?
The one marked with letter 'J'.
 
Yes, exactly.

Does anyone have any idea if the equation of initial energy written above is correct? I have doubts about the current in the inductor, since when we open the switch it disappears (gradually), doesn't it?
 
:smile: O2: Very subtle...
Rugile's post #3 seems pretty good to me: keep going !

And post #6: yes, it dampens out quickly. But the exercise only wants the total, so no need to solve the D.E.
 
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Rugile said:
Can I say that the initial energy of the system (after opening the switch) was [itex]E = \frac{CU^2}{2} + \frac{LI^2}{2}[/itex], where [itex]I = \frac{\epsilon}{R+r}[/itex] and U = epsilon = EMF ?
That looks right. That's the stored energy before the jumper to the battery is removed.

After the jumper is removed, the inductor current becomes the capacitor current, the two now being in series.
 
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