What is the dimensionless number a for a R-L circuit when the switch is closed?

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The discussion focuses on determining the dimensionless number 'a' for an R-L circuit when the switch is closed, specifically at the time when the current reaches 70% of its maximum value. Initially, there was confusion regarding the current at t=0 and the calculation of 70% of the current. It was clarified that at infinity, the current is not zero, and the correct approach involves using Kirchhoff's loop rule to derive the current equation. The final solution confirms that the current approaches ε/R as time progresses, leading to the correct identification of the dimensionless number 'a'. The problem was ultimately resolved with the assistance of other forum members.
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[SOLVED] R-L Circuit - Simple

Homework Statement



In the figure below, suppose that the switch is initially open, and at time t=0, the switch is closed. Let t1=aL/R be the time that the current through the inductor L is 70.0 percent of its value when t is infinity. Find the dimensionless number a.

http://cse.unl.edu/~ejones/Images212/LR.gif

Homework Equations



i=I_{0}e^{-(R/L)t)

The Attempt at a Solution



I tried and no luck:

Given the problem, when t is 0 the current is initially 0. So I_{0} is 0.

And I want to find .7i (70% of i) and I already know that t1=aL/R

So plugging all the info in:

.7i=0*e^{-(R/L)(aL/R)}

.7i=0

i=0

This is obviously wrong, and makes no sense to me. Help would be appreciated.
 
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Your equation is wrong. In infinity the current is not 0.

You must notice, that in infinity the voltage on inductor is 0. Hence you can calculate the current in infinity.

Than you should 'construct' right equation for the current and solve the problem (of course you can solve some differential equations instead). The one thing that is right is that the current will be exponential-like with time constant R/L
 
Okay, so is this right for finding current @ infinity?

Since voltage on inductor is 0,

L\frac{di}{dt}=0

So, using Kirchoff's loop rule:

\epsilon-L\frac{di}{dt}-iR=0

\epsilon-0-iR=0

i=\frac{\epsilon}{R}

**

EDIT: got it. Thanks!
 
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