The Principle of Superposition for Waves — Question 2

Section 16-8 · Physics pages 2534–2535

Question 2 Complete displacement cancellation can leave nonzero kinetic energy Two opposite-sign pulses on an ideal string are y = f(x −vt) −f(x + vt), with localized smooth f and F = µv2. Their centers coincide at t = 0. Opposite-sign pulses approach each other before complete overlap. (a) Find displacement, slope and transverse velocity at complete overlap. (b) Calculate total energy at that instant and compare with two separated pulses.
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Question 2 - Solution Complete displacement cancellation can leave nonzero kinetic energy Method and mathematical working Evaluate displacement, slope, and velocity separately at the overlap instant. Cancellation of the first quantity does not imply cancellation of its time derivative. y(x, 0) = 0, yx(x, 0) = 0, yt(x, 0) = −2vf′(x), u(x, 0) = 1 2µ(2vf′)2 = 2F(f′)2. Eoverlap = 2F ∫ (f′)2dx = E1 + E2, Uoverlap = 0. (a) Calculation and conclusion At t = 0, y = 0 and yx = 0, but yt = −2vf′(x). The string is momentarily straight while material elements generally move transversely. (b) Interpretation and limits Energy is entirely kinetic: E = ∫1 2µ(2vf′)2dx = 2F ∫(f′)2dx. Each separated traveling pulse has energy F ∫(f′)2dx, so total energy is conserved. Destructive displacement overlap does not destroy energy. Physical check All energy is kinetic at full cancellation. The integrated value equals the energy of the two original pulses, so a flat instantaneous string has not lost their energy.

Question 2

Complete displacement cancellation can leave nonzero kinetic energy

Two opposite-sign pulses on an ideal string are y=f(x−vt)−f(x+vt)y=f(x-vt)-f(x+vt), with localized smooth ff and F=μv2F=\mu v^2. Their centers coincide at t=0t=0.

Diagram shown in the original SVG worksheet.

  1. Find displacement, slope and transverse velocity at complete overlap.

  2. Calculate total energy at that instant and compare with two separated pulses.

Question 2 - Solution

Complete displacement cancellation can leave nonzero kinetic energy

Diagram shown in the original SVG worksheet.

Method and mathematical working

Evaluate displacement, slope, and velocity separately at the overlap instant. Cancellation of the first quantity does not imply cancellation of its time derivative.y(x,0)=0,yx(x,0)=0,yt(x,0)=−2vf′(x),u(x,0)=12μ(2vf′)2=2F(f′)2.Eoverlap=2F∫(f′)2dx=E1+E2,Uoverlap=0.\begin{aligned}y(x,0)&=0,\quad y_x(x,0)=0,\quad y_t(x,0)=-2vf^{\prime}(x),\\u(x,0)&=\tfrac12\mu(2vf^{\prime})^2=2F(f^{\prime})^2.\\[4pt]E_{\mathrm{overlap}}&=2F\int(f^{\prime})^2dx=E_1+E_2,\qquad U_{\mathrm{overlap}}=0.\end{aligned}

(a) Calculation and conclusion

At t=0t=0, y=0y=0 and yx=0y_x=0, but yt=−2vf′(x)y_t=-2vf^{\prime}(x). The string is momentarily straight while material elements generally move transversely.

(b) Interpretation and limits

Energy is entirely kinetic: E=∫12μ(2vf′)2dx=2F∫(f′)2dxE=\int\tfrac12\mu(2vf^{\prime})^2dx=2F\int(f^{\prime})^2dx. Each separated traveling pulse has energy F∫(f′)2dxF\int(f^{\prime})^2dx, so total energy is conserved. Destructive displacement overlap does not destroy energy.

Physical check

All energy is kinetic at full cancellation. The integrated value equals the energy of the two original pulses, so a flat instantaneous string has not lost their energy.