The Wave Equation — Question 2

Section 16-7 · Physics pages 2514–2515

Question 2 An arbitrary smooth translating shape satisfies the same equation Let y(x, t) = f(x −ct) for a twice-differentiable function f. A string requires ytt = v2yxx with v > 0. x v Pulse geometry and direction; the profile is schematic unless a function is given. (a) Determine which values of c allow a nontrivial curved profile. (b) Identify the exceptional profiles for which the equation does not constrain c. Explain why those exceptions cannot be used to measure a wave speed.
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Question 2 - Solution An arbitrary smooth translating shape satisfies the same equation x v Method and mathematical working Differentiate the traveling profile twice with respect to each independent variable. Compare the coefficients multiplying the same second derivative. ytt = c2f′′(x −ct), yxx = f′′(x −ct), ytt −v2yxx = (c2 −v2)f′′. f(s) = as + b ⇒f′′ = 0 ⇒ytt = yxx = 0 for any c. (a) Calculation and conclusion Differentiation gives ytt = c2f′′ and yxx = f′′. Thus (c2 −v2)f′′ = 0. If curvature is nonzero anywhere, c = ±v. (b) Interpretation and limits If f′′ = 0 everywhere, then f(ξ) = aξ + b. Both second derivatives vanish for any c. A linear ramp has no localized crest or repeating structure to track, and different descriptions reduce to changes in uniform offset velocity. Boundary and initial conditions still constrain physical realizability. Physical check For a nontrivial curved profile the coefficient must vanish, giving c = ±v. The exceptional affine profile has zero curvature and does not select a propagation speed through this test.

Question 2

An arbitrary smooth translating shape satisfies the same equation

Let y(x,t)=f(x−ct)y(x,t)=f(x-ct) for a twice-differentiable function ff. A string requires ytt=v2yxxy_{tt}=v^2y_{xx} with v>0v>0.

Diagram shown in the original SVG worksheet.

  1. Determine which values of cc allow a nontrivial curved profile.

  2. Identify the exceptional profiles for which the equation does not constrain cc. Explain why those exceptions cannot be used to measure a wave speed.

Question 2 - Solution

An arbitrary smooth translating shape satisfies the same equation

Diagram shown in the original SVG worksheet.

Method and mathematical working

Differentiate the traveling profile twice with respect to each independent variable. Compare the coefficients multiplying the same second derivative.ytt=c2f′′(x−ct),yxx=f′′(x−ct),ytt−v2yxx=(c2−v2)f′′.f(s)=as+b⇒f′′=0⇒ytt=yxx=0for any c.\begin{aligned}y_{tt}&=c^2f^{\prime\prime}(x-ct),\qquad y_{xx}=f^{\prime\prime}(x-ct),\\y_{tt}-v^2y_{xx}&=(c^2-v^2)f^{\prime\prime}.\\[4pt]f(s)=as+b&\Rightarrow f^{\prime\prime}=0\Rightarrow y_{tt}=y_{xx}=0\quad\text{for any }c.\end{aligned}

(a) Calculation and conclusion

Differentiation gives ytt=c2f′′y_{tt}=c^2f^{\prime\prime} and yxx=f′′y_{xx}=f^{\prime\prime}. Thus (c2−v2)f′′=0(c^2-v^2)f^{\prime\prime}=0. If curvature is nonzero anywhere, c=±vc=\pm v.

(b) Interpretation and limits

If f′′=0f^{\prime\prime}=0 everywhere, then f(ξ)=aξ+bf(\xi)=a\xi+b. Both second derivatives vanish for any cc. A linear ramp has no localized crest or repeating structure to track, and different descriptions reduce to changes in uniform offset velocity. Boundary and initial conditions still constrain physical realizability.

Physical check

For a nontrivial curved profile the coefficient must vanish, giving c=±vc=\pm v. The exceptional affine profile has zero curvature and does not select a propagation speed through this test.