Standing Waves — Question 8

Section 16-11 · Physics pages 2606–2607

Question 8 A relative reflection phase translates the node pattern On an unbounded uniform string, equal waves are A cos(kx −ωt) and A cos(kx + ωt + ϕ). A relative phase change shifts the spatial node pattern; the two traces represent different imposed phases. (a) Find the standing-wave form and node positions. (b) For a change ϕ : 0 →π/2, find the shift of each continuously tracked node. Could this phase change be arbitrary if a node must remain at a fixed support?
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Question 8 - Solution A relative reflection phase translates the node pattern Method and mathematical working Use the sum identity with the phase carried through both factors. Solve the spatial-zero condition for position before taking its change with phase. y = 2A cos(kx + ϕ/2) cos(ωt + ϕ/2), xn = (n + 1/2)π −ϕ/2 k , ∆xn = −∆ϕ 2k . ∆x = − π/2 2(2π/λ) = −λ/8. (a) Calculation and conclusion The sum is 2A cos(kx + ϕ/2) cos(ωt + ϕ/2). Nodes satisfy kx + ϕ/2 = (n + 1/2)π, so xn = [(n + 1/2)π −ϕ/2]/k. (b) Interpretation and limits The shift is ∆x = −∆ϕ/(2k) = −λ/8. If a fixed support must remain a node, its boundary condition constrains the allowed relative phase; one cannot change that phase independently while preserving the same standing pattern and boundary. Physical check For ∆ϕ = π/2, the shift is −λ/8. On a bounded string, an arbitrary imposed phase shift may violate an endpoint condition, so the free superposition result must be checked against the supports.

Question 8

A relative reflection phase translates the node pattern

On an unbounded uniform string, equal waves are Acos⁡(kx−ωt)A\cos(kx-\omega t) and Acos⁡(kx+ωt+ϕ)A\cos(kx+\omega t+\phi).

Diagram shown in the original SVG worksheet.

  1. Find the standing-wave form and node positions.

  2. For a change ϕ:0→π/2\phi:0\to\pi/2, find the shift of each continuously tracked node. Could this phase change be arbitrary if a node must remain at a fixed support?

Question 8 - Solution

A relative reflection phase translates the node pattern

Diagram shown in the original SVG worksheet.

Method and mathematical working

Use the sum identity with the phase carried through both factors. Solve the spatial-zero condition for position before taking its change with phase.y=2Acos⁡(kx+ϕ/2)cos⁡(ωt+ϕ/2),xn=(n+1/2)π−ϕ/2k,Δxn=−Δϕ2k.Δx=−π/22(2π/λ)=−λ/8.\begin{aligned}y&=2A\cos(kx+\phi/2)\cos(\omega t+\phi/2),\\x_n&=\frac{(n+1/2)\pi-\phi/2}{k},\qquad \Delta x_n=-\frac{\Delta\phi}{2k}.\\[4pt]\Delta x&=-\frac{\pi/2}{2(2\pi/\lambda)}=-\lambda/8.\end{aligned}

(a) Calculation and conclusion

The sum is 2Acos⁡(kx+ϕ/2)cos⁡(ωt+ϕ/2)2A\cos(kx+\phi/2)\cos(\omega t+\phi/2). Nodes satisfy kx+ϕ/2=(n+1/2)πkx+\phi/2=(n+1/2)\pi, so xn=[(n+1/2)π−ϕ/2]/kx_n=[(n+1/2)\pi-\phi/2]/k.

(b) Interpretation and limits

The shift is Δx=−Δϕ/(2k)=−λ/8\Delta x=-\Delta\phi/(2k)=-\lambda/8. If a fixed support must remain a node, its boundary condition constrains the allowed relative phase; one cannot change that phase independently while preserving the same standing pattern and boundary.

Physical check

For Δϕ=π/2\Delta\phi=\pi/2, the shift is −λ/8-\lambda/8. On a bounded string, an arbitrary imposed phase shift may violate an endpoint condition, so the free superposition result must be checked against the supports.