Inductors:
v = L[di/dt]
i = [1/L]òttovdt+i(t0)
p = [dw/dt] = vi = Li[di/dt]
w = [1/2]Li2
Series: Leq = L1+L2+L3...
Capacitors:
i = C[dv/dt]
v = [1/C]òttoidt+v(t0)
p = [dw/dt] = vi = Cv[dv/dt]
w = [1/2]Cv2
Series: Leq = L1+L2+L3...
Parallel: Ceq = C1+C2+C3...
Natural Response:
For RC circuits:
t = RC
For RL circuits:
t = [L/R]
For both: x(t) = Xoe[(-t)/(t)] ,t>0
Step Response:
x(t) = Finalvalue+(Initial-final)e[(-t)/(t)]
RLC circuits:
Series: a = [R/2L] Parallel: a = [1/2RC]
Both: w = [1/([ÖLC])] ; wd = Ö{w2-a2}
s1,2 = -a+-Ö{a2-w2}
Overdamped(both roots real and distinct): x(t) = A1es1t+A2es2t
To find Constants: x(0) = A1+A2
[dx(0)/dt] = s1A1+s2A2
Underdamped(complex roots): x(t) = B1e-atcoswdt+B2e-atsinwdt
x(0) = B1
[dx(0)/dt] = wdB2-aB1
Critically Damped(roots the same): x(t) = D1te-at+D2e-at
x(0) = D2
[dx(0)/dt] = D1-aD2
Step response of all RLC: add an Xf to each of the response equations, and to each equation for determining constants that do NOT include derivatives!