The Wave Equation — Question 9

Section 16-7 · Physics pages 2528–2529

Question 9 The differential equation contains a local energy balance For a uniform ideal string, define u = 1 2µy2 t + 1 2Fy2 x and P = −Fyxyt. The motion satisfies µytt = Fyxx. P(x) P(x + dx) dx string element Energy-flow directions across a short string interval. (a) Derive ut + Px = 0. (b) Integrate over a fixed interval [a, b] and interpret the signs of the endpoint powers.
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Question 9 - Solution The differential equation contains a local energy balance P(x) P(x + dx) dx string element Method and mathematical working Differentiate the sum of kinetic and elastic energy densities, then replace acceleration using the wave equation. The product rule identifies the spatial derivative of power. ut = µytytt + Fyxyxt = F(ytyxx + yxyxt) = F∂x(yxyt), ut + Px = 0. d dt ∫b a u dx = − ∫b a Px dx = P(a, t) −P(b, t). (a) Calculation and conclusion ut = µytytt + Fyxyxt = Fytyxx + Fyxyxt = F∂x(yxyt) = −Px. Thus increasing local stored energy corresponds to a net incoming energy flux. (b) Interpretation and limits d ∫b a u dx/dt = P(a, t) −P(b, t). Rightward power at the left endpoint enters, while rightward power at the right endpoint leaves. This conservation identity applies to arbitrary solutions, including overlapping waves, not only one sinusoidal traveler. Physical check Integrating over a fixed interval gives dE/dt = P(a) −P(b). Equal incoming and outgoing powers leave the stored energy constant, as required by conservation.

Question 9

The differential equation contains a local energy balance

For a uniform ideal string, define u=12μyt2+12Fyx2u=\tfrac12\mu y_t^2+\tfrac12F y_x^2 and P=−FyxytP=-F y_x y_t. The motion satisfies μytt=Fyxx\mu y_{tt}=F y_{xx}.

Diagram shown in the original SVG worksheet.

  1. Derive ut+Px=0u_t+P_x=0.

  2. Integrate over a fixed interval [a,b][a,b] and interpret the signs of the endpoint powers.

Question 9 - Solution

The differential equation contains a local energy balance

Diagram shown in the original SVG worksheet.

Method and mathematical working

Differentiate the sum of kinetic and elastic energy densities, then replace acceleration using the wave equation. The product rule identifies the spatial derivative of power.ut=μytytt+Fyxyxt=F(ytyxx+yxyxt)=F∂x(yxyt),ut+Px=0.ddt∫abudx=−∫abPxdx=P(a,t)−P(b,t).\begin{aligned}u_t&=\mu y_t y_{tt}+F y_x y_{xt}\\&=F(y_t y_{xx}+y_x y_{xt})=F\partial_x(y_x y_t),\\u_t+P_x&=0.\\[4pt]\frac{d}{dt}\int_a^b u\,dx&=-\int_a^bP_x\,dx=P(a,t)-P(b,t).\end{aligned}

(a) Calculation and conclusion

ut=μytytt+Fyxyxt=Fytyxx+Fyxyxt=F∂x(yxyt)=−Pxu_t=\mu y_ty_{tt}+F y_xy_{xt}=F y_ty_{xx}+F y_xy_{xt}=F\partial_x(y_xy_t)=-P_x. Thus increasing local stored energy corresponds to a net incoming energy flux.

(b) Interpretation and limits

d∫abudx/dt=P(a,t)−P(b,t)d\int_a^b u\,dx/dt=P(a,t)-P(b,t). Rightward power at the left endpoint enters, while rightward power at the right endpoint leaves. This conservation identity applies to arbitrary solutions, including overlapping waves, not only one sinusoidal traveler.

Physical check

Integrating over a fixed interval gives dE/dt=P(a)−P(b)dE/dt=P(a)-P(b). Equal incoming and outgoing powers leave the stored energy constant, as required by conservation.