How Much Energy is Dissipated in an LR Circuit When the Switch is Released?

AI Thread Summary
When the switch in an LR circuit is released, the energy dissipated through the resistors can be calculated using the formula (LI^2)/2, where I is the initial current. The correct energy dissipation is 36 J, not 81 J as initially calculated. To find this, one must first determine the current through the 6-ohm resistor before the switch opens and then apply Kirchhoff's Voltage Law (KVL) to the circuit. By solving the resulting first-order differential equation and integrating the power dissipated over time, the energy dissipated can be confirmed as 36 J. The final current being zero indicates that all energy is dissipated in the resistors.
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http://img527.imageshack.us/img527/1787/lccircuitrk6.th.gif

The switch S is closed for a long time and then released again. How much energy is dissipated through the resistors after the switch is released?

It should be (LI^2)/2 shouldn't it? Where I is the current right before the switch is released. I even integrated the R(i(t))^2 where i(t) is the current decay function of time for an RC circuit. The answer I got was 81 J but apparently the answer is 36 J? I'm deeply confused. Can someone show me how to correctly solve this if my approach is wrong?
 
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First find the current through the 6 ohm resistor in series with the inductor. Then when the switch is open, you can disregard the left hand side of the picture. The potential across the inductor is L\frac{dI}{dt}. Use that along with the value of the resistors 6 and 12 ohms to construct an equation with KVL for the case when the switch is open.

Then solve that first order DE by separation of variables. Plug in the value of I_{0} which is the initial current through the 6 ohm resistor in series with the inductor when the switch is just opened. You'll now have a decaying exponential function of t. That is the current through the circuit for t>0, assuming the switch is open at t=0. You can find the energy dissipated in the circuit by P = \frac{dE}{dt} where P is power dissipated, E is energy dissipated. Using the expression for energy dissipated in the resistors, perform an integration from t=0 to t->infinity.

You'll get 36 J.
 
Oh I see, I got 36 J. You can skip the integration using equivalent resistance to find the current in the middle branch, then do U = LI^2/2. This gives 36 J. Since the final current is 0, the energy must all be dissipated.
 
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