Transient Analysis
Time-varying currents and voltages resulting from the abrupt change of the circuit (or due to switching) are called transients.
Important in many applications
- Digital Circuits
- Timing Circuit
- Power System
Usually, transient analysis requires Ordinary Differential Equations to solve.
General Solutions
These general solutions can apply for both charging or discharging circuits.
Finding
R
When you calculate , which is really , make sure to look at it from the capacitor/inductorβs perspective, not from like the sourceβs perspective.
R is the resistance as seen from the capacitor/inductorβs perspective. Review Theveninβs Theorem
General solution for capacitors (RC Circuits)
where
- = the final value or DC steady-state value when
- = the initial value
- = Time Constant
using the above formula for , DONβT use the follow below General solution for inductors (RL Circuits) where
- = the final value or DC steady-state value when
- = the initial value
- = Time Constant, where is the thevenin resistance as seen by the inductor
using the above formula for , DONβT use the formula of capacitor for voltage.
General Guidelines for solving these problems
Capacitors Capacitors act like open-circuit at , so current becomes 0 at infinity. You solve for voltage. β ALWAYS Treat conductor like open circuit to solve for voltage
Inductors In general, for inductors, to solve , the inductor will be short circuited as the circuit stabilizes.
Remember, an inductor acts like a short circuit in DC constant current. β AWAYS Treat inductor like short circuit and solve for current
Note on
R_{th}
Just solve it the way you solve thevenin, easy.
Only exception is for finding the equivalent resistance, you treat sources and the inductor/capacitor as open-circuit as that is the definition of an equivalent/thevenin resistance.
β This got me quite confused.