Partial RL Circuit: Solving for Current in Inductor with Kirchhoff's Rules

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Homework Help Overview

The discussion revolves around analyzing a partial RL circuit using Kirchhoff's rules to determine the current in an inductor as a function of time. The circuit experiences a current pulse that varies over time, and participants are exploring how to set up the governing differential equations for the current behavior during different time intervals.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the application of Kirchhoff's rules to derive the differential equation governing the inductor's current. There are attempts to express the current in terms of time, with some uncertainty about the boundary conditions and continuity between different time intervals.

Discussion Status

The discussion is ongoing, with participants sharing their attempts to formulate the problem and expressing confusion about the relationships between the currents in the circuit. Some guidance has been offered regarding the differential equation, but there is no clear consensus on the correct expressions or the next steps to take.

Contextual Notes

Participants are working under the constraints of the problem statement, which specifies the behavior of the current pulse and the parameters of the circuit. There is a noted lack of clarity regarding the continuity of the current function across the defined time intervals.

Ithryndil
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Homework Statement


A current pulse is fed to the partial circuit shown in Figure P32.25. The current begins at zero, then becomes Imax = 7.0 A between t = 0 and t = 200 µs, and then is zero once again. Determine the current in the inductor as a function of time. Let L = 1.0 mH and R = 100 . (Use t as appropriate.) Figure

Homework Equations


...

The Attempt at a Solution



I know I need to use Kirchhoff's rules for this. I am not quite sure how to go about setting this up...I know I will have:

Emf - IR - L(dI/dt) = 0

Since there is no Emf this becomes:
L(dI/dt) = - IR

I am not sure where to go from here. I have the correct answer for [tex]0\leq[/tex] [tex]t[/tex] [tex]\leq200\mu s[/tex] being:

[tex]I(t) = 7(1 - e^{-100000t})[/tex]

I also am not sure how to proceed with finding the current for t > 200 microseconds.
 
Last edited:
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I know that Iresistor must be:

Iresistor (I2) = Iinitial(I1) - Iinductor(I3).

However, whenever I use that I can't ever seem to get the actually statement they are getting for Iinductor. I get this DE:

L(dI3/dt) = -I2*R.

When I solve that I get:

I3 = I1 + e^(-Rt/L)

That expression doesn't seem right, and is not right.
 
Ithryndil said:
Since there is no Emf this becomes:
L(dI/dt) = - IR

This is the DE you need. The boundary condition is just continuity with the earlier function you found.
 
I am not sure I follow what you mean about the earlier function. Are you talking about Kirchhoffs rule with the Emf in it?
 

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