Problem 1.39. By applying Newton's laws to the oscillations of a continuous medium, one can show that the speed of a sound wave is given by B Cs = where p is the density of the medium (mass per unit volume) and B is the bulk modulus, a measure of the medium's stiffness. More precisely, if we imagine applying an increase in pressure AP to a chunk of the material, and this increase results in a (negative) change in volume AV, then B is defined as the change in pressure divided by the magnitude of the fractional change in volume: ΔΡ B = -AV/V* This definition is still ambiguous, however, because I haven't said whether the take place isothermally or adiabatically (or in some other way). compression is

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Derive an expression for the speed of sound in an ideal gas, in terms of its temperature and average molecular mass. Compare your result to the formula for the rms speed of the molecules in the gas. Evaluate the speed of sound numerically for air at room temperature.

Problem 1.39. By applying Newton's laws to the oscillations of a continuous
medium, one can show that the speed of a sound wave is given by
B
Cs =
where p is the density of the medium (mass per unit volume) and B is the bulk
modulus, a measure of the medium's stiffness. More precisely, if we imagine
applying an increase in pressure AP to a chunk of the material, and this increase
results in a (negative) change in volume AV, then B is defined as the change in
pressure divided by the magnitude of the fractional change in volume:
ΔΡ
B =
-AV/V*
This definition is still ambiguous, however, because I haven't said whether the
take place isothermally or adiabatically (or in some other way).
compression is
Transcribed Image Text:Problem 1.39. By applying Newton's laws to the oscillations of a continuous medium, one can show that the speed of a sound wave is given by B Cs = where p is the density of the medium (mass per unit volume) and B is the bulk modulus, a measure of the medium's stiffness. More precisely, if we imagine applying an increase in pressure AP to a chunk of the material, and this increase results in a (negative) change in volume AV, then B is defined as the change in pressure divided by the magnitude of the fractional change in volume: ΔΡ B = -AV/V* This definition is still ambiguous, however, because I haven't said whether the take place isothermally or adiabatically (or in some other way). compression is
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