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Question: The velocity of sound in a gas is 300 m/s. The root mean square velocity of the molecules is of the ...

The velocity of sound in a gas is 300 m/s. The root mean square velocity of the molecules is of the order of
A. 4 m/s
B. 40 m/s
C. 400 m/s
D. 4000 m/s

Explanation

Solution

The velocity of sound in any gas is =  γRTMThe{\text{ }}velocity{\text{ }}of{\text{ }}sound{\text{ }}in{\text{ }}any{\text{ }}gas{\text{ }}is{\text{ }} = \;\sqrt {\dfrac{{\gamma RT}}{M}} ,
Where γ\gamma is the ratio of specific heats at constant pressure and constant volume.
i.e., γ=CpCv\gamma = \dfrac{{{C_p}}}{{{C_v}}},
R is the Universal gas constant,
T is the Temperature,
And M is the molecular mass.
Root mean square speed =    3RTMRoot{\text{ }}mean{\text{ }}square{\text{ }}speed{\text{ }} = \;\;\sqrt {\dfrac{{3RT}}{M}} .

Complete step by step solution:
Root mean square speed means square root of the average of the square of the velocity of the molecules of gas.
υrms=v12+v22+v32+.......vn2n{\upsilon _{rms}} = \sqrt {\dfrac{{{v_1}^2 + {v_2}^2 + {v_3}^2 +. ......{v_n}^2}}{n}} ,
n is the number of particles.
Or in other words,
As we know that Kinetic Energy for the gas molecule at temperature T is,
EK=32RT{E_K} = \dfrac{3}{2}RT,
Where R is Universal gas constant,
T is temperature in Kelvin,
EK=12mυ2{E_K} = \dfrac{1}{2}m{\upsilon ^2},
Where, m is the mass of particle,
υ\upsilon is the root mean square velocity of particle
Now, by combining these two,
We will get,
υ2=3RTM{\upsilon ^2} = \dfrac{{3RT}}{M},
υrms=3RTM{\upsilon _{rms}} = \sqrt {\dfrac{{3RT}}{M}} .

As we know that the velocity of sound of different gases is different.
Let v be the velocity of sound in air.
Let c be the Root mean square speed of air.
v=γRTMv = \sqrt {\dfrac{{\gamma RT}}{M}} (equation1)\left( {equation \to 1} \right)
c=3RTMc = \sqrt {\dfrac{{3RT}}{M}} (equation2)\left( {equation \to 2} \right)
Now, Dividing equation 1 and equation 2,
vc=γ3\dfrac{v}{c} = \sqrt {\dfrac{\gamma }{3}} (equation3)\left( {equation \to 3} \right),
Now, we have to find γ\gamma .
Here, we have to find the γ\gamma for diatomic molecules,
For diatomic molecule,
Cp=52R{C_p} = \dfrac{5}{2}R,
CP{C_P} is specific heat at constant pressure,
Cv=32R{C_v} = \dfrac{3}{2}R,
Cv{C_v} is specific heat at constant volume,

Specific heat is the amount of heat per unit mass required to raise the temperature by 11 degree Celsius.
So, γ=5R23R2\gamma = \dfrac{{\dfrac{{5R}}{2}}}{{\dfrac{{3R}}{2}}},
γ=1.4\gamma = 1.4,
Now put the value of γ\gamma in equation 3,
vc=1.43\dfrac{v}{c} = \sqrt {\dfrac{{1.4}}{3}} ,
Velocity of sound in gas = 300m/s(given)Velocity{\text{ }}of{\text{ }}sound{\text{ }}in{\text{ }}gas{\text{ }} = {\text{ }}300m/s\left( {given} \right)
c=300×31.4c = 300 \times \sqrt {\dfrac{3}{{1.4}}} ,
c=400m/s(approx)c = 400m/s(approx)

\therefore Option(C) is correct.

Note: The value of γ\gamma depends on whether the molecule is mono-atomic or diatomic. Root means square speed of a molecule depends on the temperature and molecular mass.