Circuit Theory/Convolution Integral/Examples/example49

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series LRC circuit ... find voltage across the resistor

Given that the source voltage is (2t-3t²), find voltage across the resistor.

Can do focused on V_r or: current, V_c, or V_L before converting to V_r .. Below is the V_R solution.

Outline:

Transfer Function

H(s)={\frac {V_{R}}{V_{S}}}={\frac {4}{4+s+{\frac {1}{0.25s}}}}

simplify(4/(4 + s + 1/(0.25*s)))

H(s)={\frac {4s}{s^{2}+4s+4}}

Homogeneous Solution

solve(s^2 + 4.0*s + 4.0,s)

There are two equal roots at s = -2, so the solution has the form:

V_{R_{h}}(t)=Ae^{-2t}+Bte^{-2t}+C_{1}

Particular Solution

After a long time attached to a unit step function source, the inductor has shorted and the capacitor has opened. All the drop is across the capacitor. The current is zero.

V{R_{p}}=0

This also means that C₁ has to be zero.

Initial Conditions

So far the full equation is:

V_{R}(t)=Ae^{-2t}+Bte^{-2t}

Initial current through the series leg is zero because of the assumed initial conditions of the inductor. This means V_R = 0:

V_{R}(0)=0=A

A=0

Assuming the initial voltage across the capacitor is zero, no current is flowing so the drop across the resistor is zero.

i(t)={\frac {V_{R}}{4}}

V_{L}(t)=L{di(t) \over dt}={\frac {1}{4}}((-2A+B)e^{-2t}-2Bte^{-2t})

V_{L}(0)=1={\frac {B}{4}}

B=4

V_{R}(t)=4te^{-2t}

Impulse Solution

Taking the derivative of the above get:

V_{R}\delta (t)=4e^{-2t}-8te^{-2t}

Convolution Integral

V_{R}(t)=\int _{0}^{t}(4e^{-2(t-x)}-8(t-x)e^{-2(t-x)})(2x-3x^{2})dx

f := (4*exp(-2*(t-x)) - 8*(t-x)exp(-2*(t-x)))*(2*x-3*x^2);
S :=int(f,x=0..t)

V_{R}(t)=8-8e^{-2t}-10te^{-2t}-6t

There will not be any constant since again, V_R(t) = 0 after a long time ... and the capacitor opens.

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