LC-Circuit Problem: Find I as Function of Time

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Homework Help Overview

The discussion revolves around an LC-circuit problem involving the determination of the current in the inductor as a function of time, given specific initial conditions for charge and current. The parameters include an inductance of 64mH and a capacitance of 121nF.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to apply the relationship between charge and current using trigonometric functions but encounters a contradiction with the initial conditions. Other participants suggest using differential equations or Laplace transforms, with some expressing unfamiliarity with these methods.

Discussion Status

The conversation is active, with various methods being proposed to approach the problem. Some participants are exploring traditional differential equation techniques, while others are considering the use of Laplace transforms. There is no explicit consensus on the best approach, and the discussion reflects a range of interpretations and methods.

Contextual Notes

Participants note the challenge of solving the equations given the initial conditions, with some expressing confusion about the application of Laplace transforms. The original poster's struggle with the initial conditions suggests potential constraints in the problem setup.

atlantic
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An LC-circuit has L = 64mH, C = 121nF.
At the time t=0, the charge on the condensator is 10μC and the current in the inductor is 0.3A. What is the current in the inductor as a function of time?

With:q = Q_mcos(\omega_0t+\phi) we get that: I = Q_m\omega_0cos(\omega_0t+\phi + \pi/2) (because I = dq/dt), where \omega_0 = 1/(√LC)

I thought that the initial conditions would mean that I have to solve:
q(0) = 10*10^{-6} =Q_mcos(\phi) and I(0) = 0.3 = Q_m\omega_0cos(\phi + \pi/2). But these equations have no solution(!)
 
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Here's what I do with a problem like this:

1. write the differential equation without regard to initial conditions.
2. s-transform the equation term-by-term, paying attention to
f'(t) <--> sF(s) - f(0+) and f''(t) <--> s2F(s) - sf(0+) - f'(0+).

The you just invert the ensuing transfer function back to the time domain, and you get all the i.c.'s included.

(If you haven't had the Laplace transform yet I don't know what to tell you.)
 
No, I don't know Laplace:rolleyes:
 
OK, then you have to use standard differential equations for the network, and solve in the traditional diff e manner including initial conditions.

I didn't follow you argument but I would write

i = -CdV/dt (i is + if flowing out of C)
V = Ldi/dt (i is + if flowing into L)

So i = -C(d/dt)Ldi/dt = -LCd2i/dt2 or

LCd2i/dt2 + i = 0

I.C. 1: i(0) = 0.3A
I.C. 2: di/dt(0+) = V0/L but V0 = Q0/C = 1e-5/C so di/dt(0+) = Q0/LC

So now just solve the 2nd order diff eq. with those two initial conditions.
 

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