What Initial Current Flows When S is Closed in a P241B Coaxial Cable Circuit?

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Homework Help Overview

The discussion revolves around a problem involving a P241B coaxial cable circuit, focusing on the initial current flow when a switch is closed, as well as the behavior of the current over time. The subject area includes concepts of inductance, capacitance, and circuit analysis.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the effective resistance of the circuit and its implications for initial current. Questions arise regarding the behavior of current at t=0 and t=∞, with some participants expressing uncertainty about the second part of the problem.

Discussion Status

The discussion is ongoing, with some participants providing insights into the initial conditions and potential approaches for solving the problem. There is an acknowledgment of differing levels of understanding regarding the methods suggested, particularly for the second part of the question.

Contextual Notes

Participants note that certain suggested methods may not align with their class material, indicating a potential gap in the applicability of the proposed solutions.

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Homework Statement



Type P241B coaxial cable has an inductance of 0.4 μH/m and a capacitance of 40 pF/m.
The diagram below shows a 100 m length of this cable connected to a battery and switch at the sending end and a 50Ω resistor at the receiving end.
(a) If S is closed, what initial current will flow from the battery?
(b) How long will it take before this current changes?
(c) What will be the battery current at t=∞?

s12hw4.jpg


The Attempt at a Solution



I calculated the effective resistance of the cable to be 100 ohms. Since this is in series with a 50 ohm resistor then the total resistance is 150.
 
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does this sound reasonable?

a) at t=0 current is zero because of inductor
b)
c) at t=infinity current is zero again because of capacitor

I'm stuck on B :s
 
Hah, yeah, you got the easy parts right :p

The other part is simply KVL: add up all the potentials going along the circuit to get your differential equation, and then solve the ODE. Depending on how complex your class is, you may need to solve simultaneous ODEs.
 
Thanks for the response! I don't think I know what you're talking about for the second part, though... at any rate, it doesn't relate to our class material. Might there be another way to solve this?
 

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