The Principle of Superposition for Waves — Question 6

Section 16-8 · Physics pages 2542–2543

Question 6 A force-free endpoint requires an upright reflected pulse A string occupies x < 0. Its endpoint slides vertically without friction on a massless guide, so the transverse force at x = 0 vanishes. In the small-slope model, yx(0, t) = 0. The incident pulse is f(x −vt). incident free guide An ideal free endpoint moves transversely while exerting no transverse restoring force. (a) Construct the reflected pulse and find the endpoint displacement. (b) Find endpoint power and compare the physical reason for zero flux with a fixed endpoint.
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Question 6 - Solution A force-free endpoint requires an upright reflected pulse incident free guide Method and mathematical working Use an uninverted reflected profile and differentiate it carefully: its spatial argument has derivative −1. This cancels the slope at the free end. y(0, t) = 2f(−vt), yx(0, t) = f′(−vt) −f′(−vt) = 0. yr = +f(−x −vt), P(0, t) = −F yx(0, t) | {z } 0 yt(0, t) = 0. (a) Calculation and conclusion Choose yr = f(−x −vt). Its derivative is −f′(−x −vt), canceling the incident slope at zero. The reflected pulse is upright, and endpoint displacement is 2f(−vt). (b) Interpretation and limits P = −Fyxyt = 0 because the slope, and hence transverse force, is zero. The endpoint can move. At a fixed end, zero velocity gives zero flux instead. These different boundary conditions explain the different reflection signs. Physical check The end may move with nonzero velocity, but its transverse force is zero. Thus the boundary still performs no work, and doubling endpoint displacement does not violate energy conservation.

Question 6

A force-free endpoint requires an upright reflected pulse

A string occupies x<0x<0. Its endpoint slides vertically without friction on a massless guide, so the transverse force at x=0x=0 vanishes. In the small-slope model, yx(0,t)=0y_x(0,t)=0. The incident pulse is f(x−vt)f(x-vt).

Diagram shown in the original SVG worksheet.

  1. Construct the reflected pulse and find the endpoint displacement.

  2. Find endpoint power and compare the physical reason for zero flux with a fixed endpoint.

Question 6 - Solution

A force-free endpoint requires an upright reflected pulse

Diagram shown in the original SVG worksheet.

Method and mathematical working

Use an uninverted reflected profile and differentiate it carefully: its spatial argument has derivative −1-1. This cancels the slope at the free end.y(0,t)=2f(−vt),yx(0,t)=f′(−vt)−f′(−vt)=0.yr=+f(−x−vt),P(0,t)=−Fyx(0,t)⏟0yt(0,t)=0.\begin{aligned}y(0,t)&=2f(-vt),\\y_x(0,t)&=f^{\prime}(-vt)-f^{\prime}(-vt)=0.\\[4pt]y_r&=+f(-x-vt),\qquad P(0,t)=-F\underbrace{y_x(0,t)}_{0}y_t(0,t)=0.\end{aligned}

(a) Calculation and conclusion

Choose yr=f(−x−vt)y_r=f(-x-vt). Its derivative is −f′(−x−vt)-f^{\prime}(-x-vt), canceling the incident slope at zero. The reflected pulse is upright, and endpoint displacement is 2f(−vt)2f(-vt).

(b) Interpretation and limits

P=−Fyxyt=0P=-Fy_xy_t=0 because the slope, and hence transverse force, is zero. The endpoint can move. At a fixed end, zero velocity gives zero flux instead. These different boundary conditions explain the different reflection signs.

Physical check

The end may move with nonzero velocity, but its transverse force is zero. Thus the boundary still performs no work, and doubling endpoint displacement does not violate energy conservation.