Suppose a RLC series circuit. R, L and C are in series with a battery and a switch. The switch is open. L and C are discharged.
At t=0, the switch is closed and the battery (V1) feeds the circuit.
I apply KVL to the circuit and find three equations:
CRITICALLY DAMPED
\$ V_C(t) = (At + B) \thinspace e^{-\alpha t} \$
OVERDAMPED
\$ V_C(t) = Ae^{m_1t} + Be^{m_2t} \$
UNDERDAMPED
\$ V_C(t) = e^{- \alpha t}[K_1 \thinspace Cos(\omega_d t) + K_2 \thinspace Sin(\omega_d t) ] \$
To find the coefficients of those equations I apply the two initial conditions:
- I solve the equations for t=0 and for the initial voltage across the capacitor.
- I take the derivative of the equation and solve for t=0.
Now lets talk about the current equations.
I never understood why but apparently the current equations are the same, or
CRITICALLY DAMPED
\$ i(t) = (At + B) \thinspace e^{-\alpha t} \$
OVERDAMPED
\$ i(t) = Ae^{m_1t} + Be^{m_2t} \$
UNDERDAMPED
\$ i(t) = e^{- \alpha t}[K_1 \thinspace Cos(\omega_d t) + K_2 \thinspace Sin(\omega_d t) ] \$
What are the two conditions I must use for the current equations to find the coefficients?
In the voltage equations I used the initial voltage across the capacitor and the derivative of voltage (current).
Now I have the current equations.
One condition must be to solve the equations for t=0, but what about the second condition? How do I find the coefficients of the current equations?