Interference of Waves — Question 1

Section 16-9 · Physics pages 2552–2553

Question 1 Partial constructive interference need not exceed one component amplitude Two waves travel together on the same string: y1 = A cos Φ and y2 = A cos(Φ + 2π/3), with Φ = kx −ωt. Re Im A1 A2 Two equal-amplitude contributions separated by 2π/3 in phase. (a) Find the resultant amplitude and phase. (b) Compare its mean power with the power of one wave and with the sum of the two individual powers.
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Question 1 - Solution Partial constructive interference need not exceed one component amplitude Re Im A1 A2 Method and mathematical working Add the two equal phasors by resolving them along the angle bisector. Squaring the resultant amplitude gives the power ratio for the same traveling-wave impedance. Ares = 2A cos(ϕ/2), ϕ = 2π/3, P res = P 0(Ares/A)2. y = 2A cos(π/3) cos(Φ + π/3) = A cos(Φ + π/3), P = P 0, P 1 + P 2 = 2P 0. (a) Calculation and conclusion The sum-to-product identity gives y = 2A cos(π/3) cos(Φ + π/3) = A cos(Φ + π/3). Its amplitude is A, not 2A. (b) Interpretation and limits At fixed string parameters and frequency, power is proportional to amplitude squared. The resultant power equals the power P0 of one component, while the individual powers sum to 2P0. The interference cross term is negative here, reducing the coherent total relative to that sum. Physical check The amplitude lies between zero and 2A. At this phase the cross term is negative, so the resultant power is smaller than the sum of the powers assigned to isolated contributions.

Question 1

Partial constructive interference need not exceed one component amplitude

Two waves travel together on the same string: y1=Acos⁡Φy_1=A\cos\Phi and y2=Acos⁡(Φ+2π/3)y_2=A\cos(\Phi+2\pi/3), with Φ=kx−ωt\Phi=kx-\omega t.

Diagram shown in the original SVG worksheet.

  1. Find the resultant amplitude and phase.

  2. Compare its mean power with the power of one wave and with the sum of the two individual powers.

Question 1 - Solution

Partial constructive interference need not exceed one component amplitude

Diagram shown in the original SVG worksheet.

Method and mathematical working

Add the two equal phasors by resolving them along the angle bisector. Squaring the resultant amplitude gives the power ratio for the same traveling-wave impedance.Ares=2Acos⁡(ϕ/2),ϕ=2π/3,P¯res=P¯0(Ares/A)2.y=2Acos⁡(π/3)cos⁡(Φ+π/3)=Acos⁡(Φ+π/3),P¯=P¯0,P¯1+P¯2=2P¯0.\begin{aligned}A_{\mathrm{res}}&=2A\cos(\phi/2),\qquad \phi=2\pi/3,\\\overline P_{\mathrm{res}}&=\overline P_0(A_{\mathrm{res}}/A)^2.\\[4pt]y&=2A\cos(\pi/3)\cos(\Phi+\pi/3)=A\cos(\Phi+\pi/3),\\\overline P&=\overline P_0,\qquad\overline P_1+\overline P_2=2\overline P_0.\end{aligned}

(a) Calculation and conclusion

The sum-to-product identity gives y=2Acos⁡(π/3)cos⁡(Φ+π/3)=Acos⁡(Φ+π/3)y=2A\cos(\pi/3)\cos(\Phi+\pi/3)=A\cos(\Phi+\pi/3). Its amplitude is AA, not 2A2A.

(b) Interpretation and limits

At fixed string parameters and frequency, power is proportional to amplitude squared. The resultant power equals the power P0P_0 of one component, while the individual powers sum to 2P02P_0. The interference cross term is negative here, reducing the coherent total relative to that sum.

Physical check

The amplitude lies between zero and 2A2A. At this phase the cross term is negative, so the resultant power is smaller than the sum of the powers assigned to isolated contributions.