The Principle of Superposition for Waves — Question 7

Section 16-8 · Physics pages 2544–2545

Question 7 A junction can transmit a larger displacement than the incident amplitude Two ideal strings meet at x = 0 with common tension and a massless junction. For harmonic displacement amplitudes, continuity gives 1 + r = t and force balance gives Z1(1 −r) = Z2t, where Zi = √Fµi, r = Ar/Ai and t = At/Ai. Z1 Z2 = Z1/3 incident reflected transmitted Incident, reflected, and transmitted disturbances at a string junction. (a) Solve for r, t and evaluate them for Z2 = Z1/3. (b) Use the power ratio T = (Z2/Z1)t2 and R = r2 to check conservation. Does t > 1 violate it?
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Question 7 - Solution A junction can transmit a larger displacement than the incident amplitude Z1 Z2 = Z1/3 incident reflected transmitted Method and mathematical working Solve the two boundary equations for displacement-amplitude ratios. Convert amplitudes to power ratios with the impedance factor on the transmitted side. r = Z1 −Z2 Z1 + Z2 , t = 2Z1 Z1 + Z2 , R = r2, T = Z2 Z1 t2. r = 1 −1/3 1 + 1/3 = 1 2, t = 3 2, R + T = 1 4 + 1 3 (3 2 )2 = 1. (a) Calculation and conclusion Substitution gives r = (Z1 −Z2)/(Z1 + Z2) and t = 2Z1/(Z1 + Z2). With Z2 = Z1/3, r = 1/2 and t = 3/2. The reflection is upright. (b) Interpretation and limits R = 1/4 and T = (1/3)(9/4) = 3/4, summing to one. The transmitted string has lower mechanical impedance, so a larger displacement amplitude can carry less than the incident power. Amplitude ratios are not power fractions. Physical check For the given impedances, R + T = 1. A transmitted amplitude above unity is allowed because its power is weighted by the smaller impedance.

Question 7

A junction can transmit a larger displacement than the incident amplitude

Two ideal strings meet at x=0x=0 with common tension and a massless junction. For harmonic displacement amplitudes, continuity gives 1+r=t1+r=t and force balance gives Z1(1−r)=Z2tZ_1(1-r)=Z_2t, where Zi=FμiZ_i=\sqrt{F\mu_i}, r=Ar/Air=A_r/A_i and t=At/Ait=A_t/A_i.

Diagram shown in the original SVG worksheet.

  1. Solve for r,tr,t and evaluate them for Z2=Z1/3Z_2=Z_1/3.

  2. Use the power ratio 𝒯=(Z2/Z1)t2\mathcal T=(Z_2/Z_1)t^2 and ℛ=r2\mathcal R=r^2 to check conservation. Does t>1t>1 violate it?

Question 7 - Solution

A junction can transmit a larger displacement than the incident amplitude

Diagram shown in the original SVG worksheet.

Method and mathematical working

Solve the two boundary equations for displacement-amplitude ratios. Convert amplitudes to power ratios with the impedance factor on the transmitted side.r=Z1−Z2Z1+Z2,t=2Z1Z1+Z2,R=r2,T=Z2Z1t2.r=1−1/31+1/3=12,t=32,R+T=14+13(32)2=1.\begin{aligned}r&=\frac{Z_1-Z_2}{Z_1+Z_2},\qquad t=\frac{2Z_1}{Z_1+Z_2},\\R&=r^2,\qquad T=\frac{Z_2}{Z_1}t^2.\\[4pt]r&=\frac{1-1/3}{1+1/3}=\frac12,\quad t=\frac32,\\R+T&=\frac14+\frac13\left(\frac32\right)^2=1.\end{aligned}

(a) Calculation and conclusion

Substitution gives r=(Z1−Z2)/(Z1+Z2)r=(Z_1-Z_2)/(Z_1+Z_2) and t=2Z1/(Z1+Z2)t=2Z_1/(Z_1+Z_2). With Z2=Z1/3Z_2=Z_1/3, r=1/2r=1/2 and t=3/2t=3/2. The reflection is upright.

(b) Interpretation and limits

ℛ=1/4\mathcal R=1/4 and 𝒯=(1/3)(9/4)=3/4\mathcal T=(1/3)(9/4)=3/4, summing to one. The transmitted string has lower mechanical impedance, so a larger displacement amplitude can carry less than the incident power. Amplitude ratios are not power fractions.

Physical check

For the given impedances, R+T=1R+T=1. A transmitted amplitude above unity is allowed because its power is weighted by the smaller impedance.