Forced Oscillations — Question 5

Section 31-6 · Physics pages 5080–5081

Question 5 Transient suppression takes a calculable number of decay times For an underdamped driven RLC circuit, the difference between its full charge and its sinusoidal steady state has envelope Ahe−Rt/(2L). Let L=.300 H and R=12.0 ohms. t Ah(t) Schematic; labels, not drawing lengths, specify the data. (a) Find the time required to reduce this envelope to one percent of its initial value. (b) How does the time change if R is doubled while the response remains underdamped?
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Question 5 - Solution Transient suppression takes a calculable number of decay times t Ah(t) (a) Method and calculation e−Rt/(2L) = .0100 ⇒t = (2L/R) ln 100. t = .0500 ln 100 = .230259 s . (b) Interpretation and further calculation t ∝1/R for a specified envelope ratio. t2R = tR/2 = .115129 s . Physical check The criterion concerns the transient envelope, avoiding misleading ratios at zero crossings.

Question 5

Transient suppression takes a calculable number of decay times

For an underdamped driven RLC circuit, the difference between its full charge and its sinusoidal steady state has envelope Ahe−Rt/(2L)A_h e^{-Rt/(2L)}. Let L=.300 H and R=12.0 ohms.

Diagram shown in the original SVG worksheet.

  1. Find the time required to reduce this envelope to one percent of its initial value.

  2. How does the time change if R is doubled while the response remains underdamped?

Question 5 - Solution

Transient suppression takes a calculable number of decay times

Diagram shown in the original SVG worksheet.

(a) Method and calculation

e−Rt/(2L)=.0100⇒t=(2L/R)ln⁡100.e^{-Rt/(2L)}=.0100\Rightarrow t=(2L/R)\ln100.t=.0500ln⁡100=.230259s.\boxed{t=.0500\ln100=.230259\,s}.

(b) Interpretation and further calculation

t∝1/Rfor a specified envelope ratio.t\propto1/R\quad\text{for a specified envelope ratio}.t2R=tR/2=.115129s.\boxed{t_{2R}=t_R/2=.115129\,s}.

Physical check

The criterion concerns the transient envelope, avoiding misleading ratios at zero crossings.