Current using kirchhoff's loop rule

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The discussion focuses on applying Kirchhoff's loop rule to derive the current in an RL circuit, expressed as I = (ε/R)(1 - e^(-Rt/L)). The user attempts to manipulate the equation ε = IR + L(dI/dt) but struggles with the integration process. It is suggested that they should rearrange the equation to isolate variables before integrating. An alternative approach is also mentioned, where one can verify the solution by substituting it back into the differential equation. The conversation emphasizes the importance of proper rearrangement for successful integration in solving circuit equations.
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Homework Statement


By applying kirchhoffs rules, show that the in the RL circuit is given by: I=\frac{\epsilon}{R}\left(1-e^{-\frac{Rt}{L}}\right)


Homework Equations



kirchhoff's second rule: \epsilon-IR-L\frac{dI}{dt}=0

The Attempt at a Solution


\epsilon=IR+L\frac{dI}{dt}
{\epsilon}dt=IRdt+LdI
\frac{\epsilon}{I}dt-Rdt=L\frac{1}{I}dI
then i thought to integrate both sides, LHS w.r.t t and RHS w.r.t I, but doing this on paper doesn't get to the right answer, am i going wrong somewhere with the rearranging??
 
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You can't integrate it the way you have it written. You want to get all the I's on one side and all the t's on the other first, then you can integrate it.

You could also just plug the solution in and show it satisfies the differential equation instead of solving the equation.
 
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