RC Circuits & Transient Analysis

Adapted from EECS 16B notes.

Piecewise-Constant Input

A capacitor charging to an applied voltage can be modeled by the following equation.

V(t)=V0(1etτ)V(t) = V_0(1 - e^\frac{-t}{\tau})

where τ\tau is the time constant RCRC .

Likewise, a capacitor discharging can be modeled as follows.

V(t)=V0(etτ)V(t) = V_0(e^\frac{-t}{\tau})

In terms of a piece-wise constant input, we can use the two equations to model the discharging and charging of the capacitors if we are given some initial conditions.

Solutions for General Input Functions

Given the general input function

ddtV(t)=λV(t)λu(iΔ)\frac{d}{dt}V(t) = -\lambda V(t) - \lambda u(i\Delta)

where u(iΔ)u(i\Delta) is a constant, the value of the input function at t=iΔt = i\Delta, we have a solution.

x(t)=x0eλt+0teλ(tθ)u(θ)dθx(t) = x_0e^{\lambda t} + \int_0^te^{\lambda(t-\theta)}u(\theta)d\theta

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