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Question: The speed of sound through oxygen gas at \[T\,{\text{K}}\] is \[v\,{\text{m}} \cdot {{\text{s}}^{ - ...

The speed of sound through oxygen gas at TKT\,{\text{K}} is vms1v\,{\text{m}} \cdot {{\text{s}}^{ - 1}}. At the temperature becomes 2T2T and oxygen gas dissociated into atomic oxygen, the speed of sound is:
A. Remains the same
B. Becomes 2v2v
C. Becomes 2v\sqrt 2 v
D. None of these

Explanation

Solution

Use the equation for the speed of the sound through a gas at temperature. This equation gives the relation between the adiabatic constant, gas constant, temperature of gas and molecular mass of gas.
Formula used:
The speed vv of sound through a gas at temperature TK{T_K} is
v=γRTKMv = \sqrt {\dfrac{{\gamma R{T_K}}}{M}} …… (1)
Here, γ\gamma is the adiabatic index, RR is the gas constant and MM is the molecular mass of gas.

Complete step by step answer:
The speed of sound through oxygen gas at TKT\,{\text{K}} is vms1v\,{\text{m}} \cdot {{\text{s}}^{ - 1}}.
The adiabatic constant γ\gamma for diatomic gas and monatomic gas are 75\dfrac{7}{5} and 53\dfrac{5}{3} respectively.
Rewrite equation (1) for the speed of sound through oxygen gas.
v=75RTMO2v = \sqrt {\dfrac{{\dfrac{7}{5}RT}}{{{M_{{O_2}}}}}}
Here, MO2{M_{{O_2}}} is the mass of an oxygen atom.
At the temperature becomes 2T2T and oxygen gas dissociates into atomic oxygen.
Rewrite equation (1) for the speed vv'of sound through monatomic oxygen.
v=53R(2T)MOv' = \sqrt {\dfrac{{\dfrac{5}{3}R\left( {2T} \right)}}{{{M_O}}}}
v=103RTMO\Rightarrow v' = \sqrt {\dfrac{{\dfrac{{10}}{3}RT}}{{{M_O}}}}
Here, MO{M_O} is the mass of monatomic oxygen.
The mass MO2{M_{{O_2}}} of oxygen molecules is twice as that of mass MO{M_O} of monatomic oxygen.
MO2=2MO{M_{{O_2}}} = 2{M_O}
Divide the velocity vv' of sound through monoatomic oxygen by the velocity vv of sound through oxygen molecules.
vv=103RTMO75RTMO2\dfrac{{v'}}{v} = \dfrac{{\sqrt {\dfrac{{\dfrac{{10}}{3}RT}}{{{M_O}}}} }}{{\sqrt {\dfrac{{\dfrac{7}{5}RT}}{{{M_{{O_2}}}}}} }}
vv=10RT3MO×5MO27RT\Rightarrow \dfrac{{v'}}{v} = \sqrt {\dfrac{{10RT}}{{3{M_O}}} \times \dfrac{{5{M_{{O_2}}}}}{{7RT}}}
vv=103MO×5MO27\Rightarrow \dfrac{{v'}}{v} = \sqrt {\dfrac{{10}}{{3{M_O}}} \times \dfrac{{5{M_{{O_2}}}}}{7}}
Substitute 2MO2{M_O} for MO2{M_{{O_2}}} in the above equation.
vv=103MO×5(2MO)7\Rightarrow \dfrac{{v'}}{v} = \sqrt {\dfrac{{10}}{{3{M_O}}} \times \dfrac{{5\left( {2{M_O}} \right)}}{7}}
vv=10021\Rightarrow \dfrac{{v'}}{v} = \sqrt {\dfrac{{100}}{{21}}}
v=1021v\Rightarrow v' = \dfrac{{10}}{{\sqrt {21} }}v
Therefore, the speed of sound through monoatomic oxygen is 1021v\dfrac{{10}}{{\sqrt {21} }}v.

So, the correct answer is “Option D”.

Note:
Since the oxygen molecule contains two oxygen atoms, the mass of the oxygen molecule is twice as that of the mass of monatomic oxygen.
The adiabatic constant is different for monoatomic and diatomic gas.