The Speed of a Traveling Wave — Question 1

Section 16-4 · Physics pages 2452–2453

Question 1 The sign of a constant-phase trajectory fixes direction A wave is y = A sin(6x + 18t + ϕ) in SI units, with A > 0. x q constant phase A phase feature is tracked along the spatial profile. (a) Follow a point of constant phase to find the signed propagation velocity. (b) Compare with y = −A sin(6x + 18t + ϕ). Does the leading minus sign reverse propagation?
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Question 1 - Solution The sign of a constant-phase trajectory fixes direction x q constant phase Method and mathematical working Treat the phase as a constant along the trajectory of a crest or any other identifiable phase. Differentiate this constraint with respect to time; amplitude is outside the constraint. 6x + 18t + ϕ = C, 6dx dt + 18 = 0, dx dt = −3 m/s. −A sin Φ = A sin(Φ + π), d(Φ + π) dt = 6 ˙x + 18 = 0. (a) Calculation and conclusion Constant phase requires 6x + 18t + ϕ = C, so dx/dt = −18/6 = −3 m/s. The wave travels left with speed 3 m/s. (b) Interpretation and limits The leading minus sign is a phase shift of π, since −sin Φ = sin(Φ + π). It changes displacement signs but not the slope of a constant-phase trajectory. Reversing the relative sign of the space and time terms reverses propagation. Physical check The dimensions are (rad/s)/(rad/m) = m/s. Multiplying the entire displacement by −1 preserves the same trajectory equation and therefore the same direction.

Question 1

The sign of a constant-phase trajectory fixes direction

A wave is y=Asin⁡(6x+18t+ϕ)y=A\sin(6x+18t+\phi) in SI units, with A>0A>0.

Diagram shown in the original SVG worksheet.

  1. Follow a point of constant phase to find the signed propagation velocity.

  2. Compare with y=−Asin⁡(6x+18t+ϕ)y=-A\sin(6x+18t+\phi). Does the leading minus sign reverse propagation?

Question 1 - Solution

The sign of a constant-phase trajectory fixes direction

Diagram shown in the original SVG worksheet.

Method and mathematical working

Treat the phase as a constant along the trajectory of a crest or any other identifiable phase. Differentiate this constraint with respect to time; amplitude is outside the constraint.6x+18t+ϕ=C,6dxdt+18=0,dxdt=−3m/s.−Asin⁡Φ=Asin⁡(Φ+π),d(Φ+π)dt=6ẋ+18=0.\begin{aligned}6x+18t+\phi&=C,\\6\frac{dx}{dt}+18&=0,\qquad \frac{dx}{dt}=-3\,\mathrm{m/s}.\\[4pt]-A\sin\Phi&=A\sin(\Phi+\pi),\qquad \frac{d(\Phi+\pi)}{dt}=6\dot x+18=0.\end{aligned}

(a) Calculation and conclusion

Constant phase requires 6x+18t+ϕ=C6x+18t+\phi=C, so dx/dt=−18/6=−3m/sdx/dt=-18/6=-3\,\mathrm{m/s}. The wave travels left with speed 3m/s3\,\mathrm{m/s}.

(b) Interpretation and limits

The leading minus sign is a phase shift of π\pi, since −sin⁡Φ=sin⁡(Φ+π)-\sin\Phi=\sin(\Phi+\pi). It changes displacement signs but not the slope of a constant-phase trajectory. Reversing the relative sign of the space and time terms reverses propagation.

Physical check

The dimensions are (rad/s)/(rad/m)=m/s(\mathrm{rad/s})/(\mathrm{rad/m})=\mathrm{m/s}. Multiplying the entire displacement by −1-1 preserves the same trajectory equation and therefore the same direction.