
The molar specific heat of a gas as given from the kinetic theory is $\dfrac{5}{2}R$. If it is not specified whether it is ${C_p}$ or ${C_v}$, one could conclude that the molecules of the gas-
(A) Are definitely monoatomic
(B) Are definitely rigid diatomic
(C) Are definitely non-rigid diatomic
(D) Can be monatomic or rigid diatomic
Answer
218.1k+ views
Hint: The relation between the molar specific heat of a gas at constant volume(${C_v}$) and at constant pressure(${C_p}$) is given by- ${C_p} = {C_v} + R$, Where R is the gas constant. The values corresponding to both monoatomic and diatomic gases can be calculated and compared to give the answer.
Step by step answer
According to the equipartition theorem, for a gas, each degree of freedom contributes internal energy equal to $\dfrac{1}{2}RT$ per mole. Thus,
For a monatomic gas, degree of freedom, $f = 3$
The internal energy can be given by, $U = 3 \times \dfrac{1}{2}RT = \dfrac{3}{2}RT$
The molar specific heat at constant volume, ${C_v}$ is the defined as the change in internal energy per unit temperature so can be written as, ${C_v} = \dfrac{3}{2}R$
Now, the relation between ${C_p}$ and ${C_v}$ is given by-
${C_p} - {C_v} = R$
${C_p} = {C_v} + R$
${C_p}$for a monatomic gas is given by,
${C_p} = \dfrac{3}{2}R + R$
${C_p} = \dfrac{5}{2}R$
Now a diatomic gas can have two extra degrees of freedom due to rotation along two independent axes. This makes the total degrees of freedom for a linear diatomic gas as, $f = 5$
From this we get ${C_v} = \dfrac{5}{2}R$
And the ${C_p}$ can be calculated as-
${C_p} = \dfrac{5}{2}R + R$
${C_p} = \dfrac{7}{2}R$
For a non-rigid diatomic molecule the degree of freedom is 6.
So ${C_v} = 3R$
And ${C_p} = 4R$
In monoatomic, ${C_p} = \dfrac{5}{2}R$, and in diatomic, ${C_p} = \dfrac{5}{2}R$ but in non-rigid diatomic, ${C_P} \ne {C_V} \ne \dfrac{5}{2}R$.
Since the specific heat can be both ${C_p}$ and ${C_v}$ therefore it can be a monatomic or rigid diatomic gas.
Option (D) is correct.
Note: A rigid diatomic molecule is defined as a molecule which does not possess any vibrational energy. A non-rigid diatomic molecule on the other hand has vibrational energy and thus has an extra degree of freedom, making the total number of degrees of freedom as 6.
Step by step answer
According to the equipartition theorem, for a gas, each degree of freedom contributes internal energy equal to $\dfrac{1}{2}RT$ per mole. Thus,
For a monatomic gas, degree of freedom, $f = 3$
The internal energy can be given by, $U = 3 \times \dfrac{1}{2}RT = \dfrac{3}{2}RT$
The molar specific heat at constant volume, ${C_v}$ is the defined as the change in internal energy per unit temperature so can be written as, ${C_v} = \dfrac{3}{2}R$
Now, the relation between ${C_p}$ and ${C_v}$ is given by-
${C_p} - {C_v} = R$
${C_p} = {C_v} + R$
${C_p}$for a monatomic gas is given by,
${C_p} = \dfrac{3}{2}R + R$
${C_p} = \dfrac{5}{2}R$
Now a diatomic gas can have two extra degrees of freedom due to rotation along two independent axes. This makes the total degrees of freedom for a linear diatomic gas as, $f = 5$
From this we get ${C_v} = \dfrac{5}{2}R$
And the ${C_p}$ can be calculated as-
${C_p} = \dfrac{5}{2}R + R$
${C_p} = \dfrac{7}{2}R$
For a non-rigid diatomic molecule the degree of freedom is 6.
So ${C_v} = 3R$
And ${C_p} = 4R$
In monoatomic, ${C_p} = \dfrac{5}{2}R$, and in diatomic, ${C_p} = \dfrac{5}{2}R$ but in non-rigid diatomic, ${C_P} \ne {C_V} \ne \dfrac{5}{2}R$.
Since the specific heat can be both ${C_p}$ and ${C_v}$ therefore it can be a monatomic or rigid diatomic gas.
Option (D) is correct.
Note: A rigid diatomic molecule is defined as a molecule which does not possess any vibrational energy. A non-rigid diatomic molecule on the other hand has vibrational energy and thus has an extra degree of freedom, making the total number of degrees of freedom as 6.
Recently Updated Pages
Arithmetic, Geometric & Harmonic Progressions Explained

Cartesian Form of Vector Explained: Formula, Examples & Uses

Apparent Frequency Explained: Formula, Uses & Examples

Calorimetry: Definition, Principles & Calculations

Centrifugal Force Explained: Definition, Formula & Examples

Charge in a Magnetic Field: Definition, Formula & Examples

Trending doubts
JEE Main 2026: Application Form Open, Exam Dates, Syllabus, Eligibility & Question Papers

Derivation of Equation of Trajectory Explained for Students

Hybridisation in Chemistry – Concept, Types & Applications

Understanding the Angle of Deviation in a Prism

Understanding Collisions: Types and Examples for Students

How to Convert a Galvanometer into an Ammeter or Voltmeter

Other Pages
JEE Advanced Marks vs Ranks 2025: Understanding Category-wise Qualifying Marks and Previous Year Cut-offs

Units And Measurements Class 11 Physics Chapter 1 CBSE Notes - 2025-26

NCERT Solutions For Class 11 Physics Chapter 8 Mechanical Properties Of Solids

Motion in a Straight Line Class 11 Physics Chapter 2 CBSE Notes - 2025-26

NCERT Solutions for Class 11 Physics Chapter 7 Gravitation 2025-26

Understanding Atomic Structure for Beginners

