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Another way to think of sound

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Presentation on theme: "Another way to think of sound"— Presentation transcript:

1 Another way to think of sound
Pressure Waves Another way to think of sound § 16.1–16.2

2 Speed of Sound Restoring force inertia v =

3 Fractional volume change
Sound in a Fluid Restoring force = pressure Pressure responds to deformation Bulk modulus B −Pressure change Fractional volume change −p DV/V0 B = = Units = pressure units = Pa

4 Sound in a Solid Rod Restoring force = tensile stress
Stress = Force/Area (in one dimension) Strain = Fractional elongation Young’s modulus Y Longitudinal stress Longitudinal strain Y = F/A DL/L0 = Units = N/m2 = Pa

5 Group Work Draw several cycles of a longitudinal wave train.
What force accelerates the particles? Identify where pressure is high or low. Identify the acceleration directions at different positions along a phase.

6 Group Work / CPS For any wave/oscillation:
What is the particle speed when the displacement magnitude is greatest? A. Maximum. B. Zero. C. ? What is the displacement magnitude when the particle speed is greatest?

7 Group Work / CPS For any wave/oscillation:
What is the particle acceleration when the particle speed is greatest? A. ±Maximum. B. Zero. C. ? What is the particle speed when the particle acceleration is greatest? A. Maximum. B. Zero. C. ?

8 Group Work / CPS For a sound wave:
What is the particle acceleration where the pressure excursion is greatest? A. Maximum. B. Zero. C. ?

9 Longitudinal Wave Formula
y(x, t) = A cos(kx − wt) y = displacement from equilibrium position x Particle position = x + y

10 Longitudinal Wave Pressure
y(x, t) = A cos(kx − wt) Find an expression for pressure excursion p(x, t) In a fluid, p = − bulk modulus fractional volume change What is the fractional volume change of a segment of the fluid?

11 Longitudinal Wave Pressure
Does the net force on a segment really relate to the pressure gradient?

12 Lab 12 Ignore the question on p. 112 Replace Postlab question 5 with:
Calculate Young’s modulus Y for brass, steel, and aluminum from the literature values of density and speed of sound. Compare these to the literature values of Y for these materials. The values are substantially different! What might these differences mean?


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