Solving LR Circuit with Laplace Transform I have a RLC circuit where the capacitor is connected in parallel with a resistance and inductance in series. The battery is connected "in parallel" with the capacitor and the RL branches. At t=0 the battery is disconnected from the circuit. I need to find the voltage across each element using the Laplace transform.
Here’s what I did:
$$ E = RI + L\frac{dI}{dt} $$
Taking the transform I arrive at:
$$\frac{E}{s} = R ℒ(I) + L(s ℒ(I) - I_0)$$
With $I(t=0) = I_0$
$$ => ℒ(I) = \frac{E/L}{s(R/L + s)} + \frac{I_0/L}{R/L + s} $$
Which gives
$$I(t) = \frac{E}{R} + [I_0 - \frac{E}{R}]e^{-Rt/L}$$
The thing is this result looks kind of weird and I feel like I did something wrong. Could anybody let know what I should do about this?
 A: You got the very first equation wrong. The equation
$$E = RI + L\frac{dI}{dt}$$
would describe the time evolution of the inductor's current for $t<0$, not for $t>0$. 
For $t<0$, one usually assumes that the circuit is at steady-state: this assumption is used to calculate the initial conditions, in this case, the voltage across the capacitor and the current through the inductor. The initial conditions are thus $v_C(0+)=v_C(0-)=E$, for the capacitor voltage $v_C(t)$,  and $i_L(0+)=i_L(0-)=E/R$, for the inductor current $i_L(t)$, where $v_C(0-) = \lim_{t\rightarrow 0^-} v_C(t)$, $v_C(0+) =\lim_{t\rightarrow 0^+} v_C(t)$, etc. Recall that the voltage across a capacitor and the current through an inductor cannot change instantaneously.
For $t>0$ you should write the differential equation associated to the circuit realized at $t>0$, which is composed of three series-connected elements, and then transform it in the Laplace domain with the initial conditions I described in the previous paragraph.
