Standing Waves — Question 6

Section 16-11 · Physics pages 2602–2603

Question 6 Zero mean power permits instantaneous energy exchange within a loop For y = B sin(kx) cos ωt, use P = −Fyxyt with rightward flux positive. P(x) P(x + dx) dx string element Instantaneous energy can move across an internal cut of a standing wave even when cycle-averaged flow vanishes. (a) Derive the instantaneous power and its time average. (b) Locate positions where power vanishes for all time. Does zero mean flux imply that every interior point exchanges no energy with its neighbors?
Show solutionHide solution
Question 6 - Solution Zero mean power permits instantaneous energy exchange within a loop P(x) P(x + dx) dx string element Method and mathematical working Multiply the spatial and temporal derivatives in the signed power formula. Use double-angle identities to expose the separate spatial and temporal zero factors. P = −F(Bk cos kx cos ωt)(−Bω sin kx sin ωt) = FB2kω 4 sin(2kx) sin(2ωt). ⟨P⟩= 1 T ∫T 0 P(x, t) dt = 0, sin 2kx = 0 ⇒P(x, t) = 0. (a) Calculation and conclusion P = FB2kω sin(kx) cos(kx) sin ωt cos ωt = (FB2kω/4) sin(2kx) sin(2ωt). Its average over a period is zero. (b) Interpretation and limits Permanent zero-flux positions have sin(2kx) = 0, including both displacement nodes and antinodes. Between them the flux reverses sign periodically, redistributing energy locally. Zero cycle-averaged transport is compatible with nonzero instantaneous transfer. Physical check The time average of sin(2ωt) is zero. At nodes and antinodes the spatial factor also vanishes, so power there is zero instantaneously, not merely on average.

Question 6

Zero mean power permits instantaneous energy exchange within a loop

For y=Bsin⁡(kx)cos⁡ωty=B\sin(kx)\cos\omega t, use P=−FyxytP=-F y_xy_t with rightward flux positive.

Diagram shown in the original SVG worksheet.

  1. Derive the instantaneous power and its time average.

  2. Locate positions where power vanishes for all time. Does zero mean flux imply that every interior point exchanges no energy with its neighbors?

Question 6 - Solution

Zero mean power permits instantaneous energy exchange within a loop

Diagram shown in the original SVG worksheet.

Method and mathematical working

Multiply the spatial and temporal derivatives in the signed power formula. Use double-angle identities to expose the separate spatial and temporal zero factors.P=−F(Bkcos⁡kxcos⁡ωt)(−Bωsin⁡kxsin⁡ωt)=FB2kω4sin⁡(2kx)sin⁡(2ωt).⟨P⟩=1T∫0TP(x,t)dt=0,sin⁡2kx=0⇒P(x,t)=0.\begin{aligned}P&=-F(Bk\cos kx\cos\omega t)(-B\omega\sin kx\sin\omega t)\\&=\frac{FB^2k\omega}{4}\sin(2kx)\sin(2\omega t).\\[4pt]\langle P\rangle&=\frac1T\int_0^T P(x,t)\,dt=0,\qquad\sin2kx=0\Rightarrow P(x,t)=0.\end{aligned}

(a) Calculation and conclusion

P=FB2kωsin⁡(kx)cos⁡(kx)sin⁡ωtcos⁡ωt=(FB2kω/4)sin⁡(2kx)sin⁡(2ωt)P=FB^2k\omega\sin(kx)\cos(kx)\sin\omega t\cos\omega t=(FB^2k\omega/4)\sin(2kx)\sin(2\omega t). Its average over a period is zero.

(b) Interpretation and limits

Permanent zero-flux positions have sin⁡(2kx)=0\sin(2kx)=0, including both displacement nodes and antinodes. Between them the flux reverses sign periodically, redistributing energy locally. Zero cycle-averaged transport is compatible with nonzero instantaneous transfer.

Physical check

The time average of sin⁡(2ωt)\sin(2\omega t) is zero. At nodes and antinodes the spatial factor also vanishes, so power there is zero instantaneously, not merely on average.