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Question: For air at room temperature the atmospheric pressure is \(1.0 \times {10^5}N{m^{ - 2}}\) and density...

For air at room temperature the atmospheric pressure is 1.0×105Nm21.0 \times {10^5}N{m^{ - 2}} and density of air is 1.2kgm31.2kg{m^{ - 3}}. For a tube of length 1.0m closed at one end the lowest frequency generated is 84Hz84Hz. The value of γ (ratio of two specific heats) for air is:
A) 2.12.1
B) 1.51.5
C) 1.81.8
D) 1.41.4

Explanation

Solution

Use the Newton’s formula for speed of sound and laplace’s correction that establishes a relationship between speed of sound wrt pressure, temperature and ratio of specific heats.

Complete step by step answer:
We know that v=γPρv = \sqrt {\dfrac{{\gamma P}}{\rho }} , (According to Newton’s formula for speed of sound)
Where v is the velocity of sound,
γ\gamma is the ratio of the two specific heats (Cp&Cv{C_p}\& {C_v}) of air,
P is the pressure and
ρ\rho is the density of air.
Now, for calculation v, we can use the relation among frequency(f), tube length(l), and velocity of air(v), and that relation is:
f=v4lf = \dfrac{v}{{4l}},
On putting values and solving, we get,
84=v4×184 = \dfrac{v}{{4 \times 1}}
On solving it we get v as,
v=84×4=336ms1v = 84 \times 4 = 336m{s^{ - 1}}

Putting all values in Newton’s formula, we get,
336=γ×1.0×1051.2336 = \sqrt {\dfrac{{\gamma \times 1.0 \times {{10}^5}}}{{1.2}}}
Squaring on both sides, we get,
(336)2=γ×1051.2{\left( {336} \right)^2} = \dfrac{{\gamma \times {{10}^5}}}{{1.2}}
On further solving we get gamma as,
γ=(336)2×1.2105 γ1.351.4  \gamma = \dfrac{{{{\left( {336} \right)}^2} \times 1.2}}{{{{10}^5}}} \\\ \gamma \approx 1.35 \approx 1.4 \\\

So, the correct option is (D).

Note: In the tubes that are open from one end and close at other end, at close end, amplitude of the wave will be minimum, that is, 0 and at the open end, amplitude of wave will be maximum, that’s why we use the formula f=v4lf = \dfrac{v}{{4l}}, as the wavelength becomes 4 times of length of tube.