Traveling Sound Waves — Question 6

Section 17-3 · Physics pages 2682–2683

Question 6 A pulse accelerates material according to its pressure slope At t = 0 a rightward pressure pulse is p(x, 0) = P exp(−x2/ℓ2), with P = 2.0 Pa, ℓ= 0.50 m, ρ0 = 1.25 kg/m3 and c = 320 m/s. Use u = p/(ρ0c) and ut = −px/ρ0. x p Gaussian pressure snapshot; the horizontal origin in the calculation is the pulse center. (a) Find particle velocity and acceleration at the pulse center. (b) Find where the acceleration magnitude is greatest and evaluate it. State the acceleration signs on both sides of the center.
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Question 6 - Solution A pulse accelerates material according to its pressure slope x p (a) Method and calculation At the pressure maximum, u(0, 0) = 2 1.25(320) = 0.0050 m/s, px(0, 0) = 0, ut(0, 0) = 0. The material is moving there but its instantaneous acceleration vanishes. (b) Interpretation and further calculation Differentiation yields ut(x, 0) = 2Px ρ0ℓ2 e−x2/ℓ2. For x > 0, maximize xe−x2/ℓ2; its derivative vanishes when 1 −2x2/ℓ2 = 0. Thus |x| = ℓ/ √ 2 = 0.3536 m, |ut|max = √ 2P ρ0ℓe−1/2 = 2.745 m/s2. Acceleration is positive ahead (x > 0) and negative behind (x < 0). Physical check The center has maximum velocity but zero acceleration, just as a smooth velocity pulse requires. Units follow from pressure gradient divided by density.

Question 6

A pulse accelerates material according to its pressure slope

At t=0t=0 a rightward pressure pulse is p(x,0)=Pexp⁡(−x2/ℓ2)p(x,0)=P\exp(-x^2/\ell^2), with P=2.0PaP=2.0\,\mathrm{Pa}, ℓ=0.50m\ell=0.50\,\mathrm m, ρ0=1.25kg/m3\rho_0=1.25\,\mathrm{kg/m^3} and c=320m/sc=320\,\mathrm{m/s}. Use u=p/(ρ0c)u=p/(\rho_0c) and ut=−px/ρ0u_t=-p_x/\rho_0.

Diagram shown in the original SVG worksheet.

  1. Find particle velocity and acceleration at the pulse center.

  2. Find where the acceleration magnitude is greatest and evaluate it. State the acceleration signs on both sides of the center.

Question 6 - Solution

A pulse accelerates material according to its pressure slope

Diagram shown in the original SVG worksheet.

(a) Method and calculation

At the pressure maximum,u(0,0)=21.25(320)=0.0050m/s,px(0,0)=0,ut(0,0)=0.u(0,0)=\frac{2}{1.25(320)}=0.0050\,\mathrm{m/s},\quad p_x(0,0)=0,\quad u_t(0,0)=0.The material is moving there but its instantaneous acceleration vanishes.

(b) Interpretation and further calculation

Differentiation yieldsut(x,0)=2Pxρ0ℓ2e−x2/ℓ2.u_t(x,0)=\frac{2Px}{\rho_0\ell^2}e^{-x^2/\ell^2}.For x>0x>0, maximize xe−x2/ℓ2x e^{-x^2/\ell^2}; its derivative vanishes when 1−2x2/ℓ2=01-2x^2/\ell^2=0. Thus|x|=ℓ/2=0.3536m,|ut|max=2Pρ0ℓe−1/2=2.745m/s2.|x|=\ell/\sqrt2=0.3536\,\mathrm m,\quad |u_t|_{\max}=\frac{\sqrt2P}{\rho_0\ell}e^{-1/2}=2.745\,\mathrm{m/s^2}.Acceleration is positive ahead (x>0x>0) and negative behind (x<0x<0).

Physical check

The center has maximum velocity but zero acceleration, just as a smooth velocity pulse requires. Units follow from pressure gradient divided by density.