Solving a First Order Inhomogeneous ODE for a Regular LR Circuit with AC Voltage

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The discussion focuses on solving a first-order inhomogeneous ordinary differential equation (ODE) for a regular LR circuit with AC voltage. The initial approach involved using undetermined coefficients and Cramer's Rule, leading to a general solution comprising exponential, cosine, and sine terms. A key insight was the application of the cosine difference identity to express the solution in a desired form, with a right triangle analogy to relate parameters R, ω, and L. A mistake was identified in evaluating the coefficient of the exponential term, which was corrected by acknowledging the sine term's behavior at t=0. Ultimately, the participant successfully reformulated their solution and expressed gratitude for the assistance received.
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For a regular LR circuit (L and R in series) and with a AC voltage:

R8yRjNY.jpg


I tried to derive the solution myself.

https://www.dropbox.com/s/jmsu9j0vt91ze8x/LRcircuit.jpg

So first I solved with undetermined coefficients, plugged them in, and then solved with Cramer's Rule.

Then I added the term (the solution for the homogeneous case) with the solution I got with undertermined coefficients.

Then I used initial value: the current i(t) at t=0 is 0.

Then I got the general solution: an exponential term, a cosine term and a sine term. But my solution is quite different from the book.


Can anyone help me?
 
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Your solutions looks correct.

To get it into the above form you have to use the cos difference identity...

\cos {\left(\left(\omega t + \phi\right) - \theta\right)}=\cos {\left(\omega t + \phi\right)}\cos {\theta}+\sin {\left(\omega t + \phi\right)} \sin {\theta}

The trick is to figure out what \theta is in terms of R,\omega, L. To do this think of a right triangle with sides R and \omega L.
 
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the_wolfman said:
Your solutions looks correct.

To get it into the above form you have to use the cos difference identity...

\cos {\left(\left(\omega t + \phi\right) - \theta\right)}=\cos {\left(\omega t + \phi\right)}\cos {\theta}+\sin {\left(\omega t + \phi\right)} \sin {\theta}

The trick is to figure out what \theta is in terms of R,\omega, L. To do this think of a right triangle with sides R and \omega L.

I made a mistake in my solution bye the way.

In evaluating the coefficient of C of the exponential term, when I took t = 0 I let the sine term vanishes but that doesn't vanishes sin (wt + q) it become sin (q). I was thinking about sin (wt) becomes zero, yes but not with a phase angle between the brackets. Stupid mistake.

This the correct one:

https://www.dropbox.com/s/ne1wo9wknk3s1mw/20140711_121219~2.jpg

Then I used a numerical example to comparize mine solution with the one for the book.

No idea how I will get it in that form from the book. :) I'm going to try later this day. Thanks for your identity.Edit: I got it! Thanks again for your identity. I will post solution to be complete soon. :)
 
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