Types of Waves — Question 7

Section 16-1 · Physics pages 2404–2405

Question 7 A traveling boundary can imitate a pulse without local wave dynamics A rigid stencil with a bright triangular opening is translated over a screen at 3.0 m/s. Screen pixels brighten and darken as the opening passes. A triangular disturbance on a rope also advances at 3.0 m/s. screen An externally moved aperture sweeps illumination across a stationary screen. (a) Identify what the two observed records have in common. (b) Explain why identical brightness and displacement profiles do not demonstrate the same physical transmission mechanism. What additional information is needed?
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Question 7 - Solution A traveling boundary can imitate a pulse without local wave dynamics screen Method and mathematical working Compare the mathematical record with the causal mechanism. A field of the form q(x, t) = f(x −vt) describes translation but does not, by itself, specify what generates that translation. q(x, t) = f(x −vt), qt = −vf′, qx = f′, qt + vqx = 0 for either translating record. (a) Calculation and conclusion At fixed positions both produce delayed versions of a passing profile, with equal pattern speeds. The time records alone can be mathematically similar even though brightness and rope displacement are different measured quantities. (b) Interpretation and limits The stencil imposes the screen pattern externally; neighboring pixels need not pass the brightening to one another. The rope pattern arises from local inertia and tension. One must identify the field, coupling and energy source before classifying the physical mechanism; resemblance of moving shapes is insufficient. Physical check The illumination can be imposed independently at each screen point from a moving external source. A rope pulse instead evolves through forces between neighboring pieces of material. The same profile is compatible with different mechanisms.

Question 7

A traveling boundary can imitate a pulse without local wave dynamics

A rigid stencil with a bright triangular opening is translated over a screen at 3.0m/s3.0\,\mathrm{m/s}. Screen pixels brighten and darken as the opening passes. A triangular disturbance on a rope also advances at 3.0m/s3.0\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Identify what the two observed records have in common.

  2. Explain why identical brightness and displacement profiles do not demonstrate the same physical transmission mechanism. What additional information is needed?

Question 7 - Solution

A traveling boundary can imitate a pulse without local wave dynamics

Diagram shown in the original SVG worksheet.

Method and mathematical working

Compare the mathematical record with the causal mechanism. A field of the form q(x,t)=f(x−vt)q(x,t)=f(x-vt) describes translation but does not, by itself, specify what generates that translation.q(x,t)=f(x−vt),qt=−vf′,qx=f′,qt+vqx=0for either translating record.\begin{aligned}q(x,t)&=f(x-vt),\qquad q_t=-vf^{\prime},\quad q_x=f^{\prime},\\q_t+vq_x&=0\quad\text{for either translating record}.\end{aligned}

(a) Calculation and conclusion

At fixed positions both produce delayed versions of a passing profile, with equal pattern speeds. The time records alone can be mathematically similar even though brightness and rope displacement are different measured quantities.

(b) Interpretation and limits

The stencil imposes the screen pattern externally; neighboring pixels need not pass the brightening to one another. The rope pattern arises from local inertia and tension. One must identify the field, coupling and energy source before classifying the physical mechanism; resemblance of moving shapes is insufficient.

Physical check

The illumination can be imposed independently at each screen point from a moving external source. A rope pulse instead evolves through forces between neighboring pieces of material. The same profile is compatible with different mechanisms.