Forced Oscillations — Question 6

Section 31-6 · Physics pages 5082–5083

Question 6 Switching on a resonant source requires a natural transient to enforce zero initial current An underdamped series RLC circuit starts at q=i=0 when vs = Vp cos ω0t is applied. Let α = R/(2L) and ωd = √ ω2 0 −α2. ∼ vs(t) R C L q i = ˙q Schematic; labels, not drawing lengths, specify the data. (a) Combine the resonant steady charge with a homogeneous term to meet both initial conditions. (b) Check the initial current derivative against the circuit equation.
Show solutionHide solution
Question 6 - Solution Switching on a resonant source requires a natural transient to enforce zero initial current ∼ vs(t) R C L q i = ˙q (a) Method and calculation qs = Vp Rω0 sin ω0t, qh = e−αt(A cos ωdt + B sin ωdt). q = Vp Rω0 sin ω0t −Vp Rωd e−αt sin ωdt . (b) Interpretation and further calculation q(0) = 0, ˙q(0) = Vp/R −Vp/R = 0. ¨q(0) = 2αVp/R = Vp/L . Physical check Using the steady sinusoid alone would incorrectly create an instantaneous current jump.

Question 6

Switching on a resonant source requires a natural transient to enforce zero initial current

An underdamped series RLC circuit starts at q=i=0 when vs=Vpcos⁡ω0tv_s=V_p\cos\omega_0t is applied. Let α=R/(2L)\alpha=R/(2L) and ωd=ω02−α2\omega_d=\sqrt{\omega_0^2-\alpha^2}.

Diagram shown in the original SVG worksheet.

  1. Combine the resonant steady charge with a homogeneous term to meet both initial conditions.

  2. Check the initial current derivative against the circuit equation.

Question 6 - Solution

Switching on a resonant source requires a natural transient to enforce zero initial current

Diagram shown in the original SVG worksheet.

(a) Method and calculation

qs=VpRω0sin⁡ω0t,qh=e−αt(Acos⁡ωdt+Bsin⁡ωdt).q_s=\frac{V_p}{R\omega_0}\sin\omega_0t,\quad q_h=e^{-\alpha t}(A\cos\omega_dt+B\sin\omega_dt).q=VpRω0sin⁡ω0t−VpRωde−αtsin⁡ωdt.\boxed{q=\frac{V_p}{R\omega_0}\sin\omega_0t-\frac{V_p}{R\omega_d}e^{-\alpha t}\sin\omega_dt}.

(b) Interpretation and further calculation

q(0)=0,q̇(0)=Vp/R−Vp/R=0.q(0)=0,\quad\dot q(0)=V_p/R-V_p/R=0.q̈(0)=2αVp/R=Vp/L.\boxed{\ddot q(0)=2\alpha V_p/R=V_p/L}.

Physical check

Using the steady sinusoid alone would incorrectly create an instantaneous current jump.