Oscillations in an LC circuit (Question from Irodov)

AI Thread Summary
The discussion centers on solving a problem related to oscillations in an LC circuit, where the original figure and attempts at solutions were missing. Participants explore the relationship between angular frequency (ω), energy conservation, and the effects of changing distance (d) between plates in the circuit. One user concluded that their initial assumption of constant total energy in LC oscillations was incorrect and derived a new expression for maximum charge (Qmax) as a function of distance. They noted that while certain energy forms remained unchanged, the assumption of no current change might be flawed. The conversation highlights the complexities of energy dynamics in oscillating circuits and the importance of accurate assumptions in problem-solving.
Anubhav
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Homework Statement
1. The problem statement, all variables and given/known data
In an oscillating circuit consisting of of a parallel-plate capacitor and an inductance coil with negligible active resistance the oscillations with energy are sustained. The capacitor plates were slowly drawn apart to increase the scillation frequency -fold. What work was done in the process?
Relevant Equations
Variables have meaning as usual
€=permitivity of vaccum
Energy in LC oscillations =W
Energy of charged capacitor=(Q^2)/2C
Force between plates of parallel plate capacitor=(Q^2)/2€A
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For those who want to read it without breaking their neck ...

I can also decipher another relevant equation (## \ \omega = \displaystyle {1\over\sqrt{LC}}\ ##)
So inceasing ##\omega## n times means changing ##\ d \rightarrow n^2d\ ##.
Unclear to me what is conserved -- is ##\ q\ ## the same as ##\ Q_{\text{max}}\ ## ? and is that invariant ?
Then where does the mechanical work energy go ?

##\ ##
 
I'm sorry for inconvenience ..I shall delete this thread and reframe the entire Q properly again
 
Pinging @DaveE

Congratulations with the badge ! I'm sure there is no broom, and I'm certain they don't have cookies either (my clumsy way to distinguish you from @davenn)​
@Anubhav shouldn't apologize too much. Plenty effort demonstrated. I'm just filing away at his (her?) assumptions to test them. Can you handle this one in a more didactically responsible way :smile: ?

I ask myself: Would there be much difference between this case of changing ##d## and the DC case ?

##\ ##
 
BvU said:
Pinging @DaveE

Congratulations with the badge ! I'm sure there is no broom, and I'm certain they don't have cookies either (my clumsy way to distinguish you from @davenn)​
@Anubhav shouldn't apologize too much. Plenty effort demonstrated. I'm just filing away at his (her?) assumptions to test them. Can you handle this one in a more didactically responsible way :smile: ?

I ask myself: Would there be much difference between this case of changing ##d## and the DC case ?

##\ ##
Hello sir..Thanks for your I read your reply and gave it a thought again...
Also I have posted a typed image of Question as certain elements were missing in Q which I wrote
I am happy to inform you that after discussion with my friends I was able to solve it and got the right answer.
Actually I had assumed the Total energy of LC oscillations to be constant. Obviously that was wrong.
In my another attempt I wrote Change in energy of LC oscillations [i.e change in Qmax^2/(2C)] as function of integration of F(x).dx (where x is distance between plates)
Differentiation of this leads to a differential equation solving which gives Qmax as function of x..
Then change in energy of LC oscillations gives Total work done.
Ans comes out to be W(n-1)
Screenshot_20210428-183828~2.png
 
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Assumption: current does not change. (No dissipation, is like amperian currents in a permanent magnet).
So:
## V_C \rightarrow nV_C ##
## V^2_C \rightarrow n^2V^2_C ##
## C \rightarrow C/n^2 ##
So ## 1/2 ~CV_C^2 ## is unchanged; inductance energy is unchanged; circuit energy is unchanged; work = 0.

Probably wrong somewhere.Probably assumption of no current change.
 
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