
Determine the value of $ {C_p},{C_v} $ and $ \gamma $ for a monatomic, diatomic and polyatomic gas.
Answer
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Hint: In a thermodynamic system, $ {C_p} $ is the amount of heat energy absorbed or released by a unit mass of a given substance with the change in temperature at a constant pressure. $ {C_v} $ is the amount of heat energy transferred between a system and its surroundings at a constant volume. $ \gamma $ is the ratio of $ {C_p} $ and $ {C_v} $
Complete answer:
The degree of freedom of a molecule will affect the value of all the specific heat constants.
For any molecule the degrees of freedom is given by the equation:
$ f = 3N - m $
Where f is the degree of freedom
N is the number of particles in the given system/molecule
m is the number of constraints.
So for the given type of molecules we can say that:
Now we can say that the specific heat constants are related to the degree of freedom by the following equations:
$ \Rightarrow {C_p} = R(1 + \dfrac{1}{2}f) $
$ \Rightarrow {C_v} = \dfrac{1}{2}f \times R $
$ \Rightarrow \gamma = 1 + \dfrac{2}{f} $
Therefore we can substitute the values of f in the equations and obtain the value of all the constants for monoatomic, diatomic and polyatomic gas.
Note:
For gas with molecules having higher numbers of atomicity, the degree of freedom would vary even more because there are a large number of arrangements that are possible. This will mean that there will be more degrees of freedom with each type of molecule. Thus for such types of gases a known degree of freedom can be used to figure out the specific molar heats and their ratios, which will always be decreasing with increasing atomicity of the molecule.
Complete answer:
The degree of freedom of a molecule will affect the value of all the specific heat constants.
For any molecule the degrees of freedom is given by the equation:
$ f = 3N - m $
Where f is the degree of freedom
N is the number of particles in the given system/molecule
m is the number of constraints.
So for the given type of molecules we can say that:
| Type of molecule | Degrees of freedom |
| Monoatomic molecule | 3 (N=1, m=0) |
| Diatomic molecule | 5 (N=2, m=1) |
| Polyatomic molecule | >6 |
Now we can say that the specific heat constants are related to the degree of freedom by the following equations:
$ \Rightarrow {C_p} = R(1 + \dfrac{1}{2}f) $
$ \Rightarrow {C_v} = \dfrac{1}{2}f \times R $
$ \Rightarrow \gamma = 1 + \dfrac{2}{f} $
Therefore we can substitute the values of f in the equations and obtain the value of all the constants for monoatomic, diatomic and polyatomic gas.
| Type of Gas molecule | Degree of freedom f | $ {C_p} $ | $ {C_v} $ | $ \gamma $ |
| Monoatomic | 3 | $ \dfrac{5}{2}R $ | $ \dfrac{3}{2}R $ | $ \dfrac{5}{3} $ |
| Diatomic | 5 | $ \dfrac{7}{2}R $ | $ \dfrac{5}{2}R $ | $ \dfrac{7}{5} $ |
| Triatomic (A case of polyatomic) | 7 (where N=3 and m=2) | $ \dfrac{9}{2}R $ | $ \dfrac{7}{2}R $ | $ \dfrac{9}{7} $ |
Note:
For gas with molecules having higher numbers of atomicity, the degree of freedom would vary even more because there are a large number of arrangements that are possible. This will mean that there will be more degrees of freedom with each type of molecule. Thus for such types of gases a known degree of freedom can be used to figure out the specific molar heats and their ratios, which will always be decreasing with increasing atomicity of the molecule.
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