11P13
Kinetic Theory of Gases
Learning Objectives
Equipartition law of Energy and Energy of Gases
Behaviour of Gases and Their Kinetics
11P13.1
Behaviour of Gases and Their Kinetics
Learning Objectives
Pressure Calculation Applied by Gas
Postulates of Kinetic Theory of Gases
Kinetic Interpretation of Temperature
Maxwell’s Speed Distribution Law
11P13.1
CV 1
Postulates of Kinetic Theory and Maxwell’s Speed Distribution Law
Postulates of Kinetic Theory of Gases :
Postulates of Kinetic Theory of Gases :
Postulates of Kinetic Theory of Gases :
Postulates of Kinetic Theory of Gases :
Number of Particles
Speed of Particles
Postulates of Kinetic Theory of Gases :
Number of Particles
Speed of Particles
Maxwell’s Speed Distribution Law :
In a given mass of gas, the velocities of all molecules are not the same, even when the bulk parameters like pressure, volume and temperature are fixed.
Collisions changes the direction and the speed of molecules.
Distributions are very important when we are dealing with system containing large number of objects.
Equation of Maxwell’s Speed Distribution :
Maxwell’s Speed Distribution Law :
It is the speed attained by maximum number of gas molecules.
By solving given equation
Most Probable Speed
Maxwell’s Speed Distribution Law :
For Average Speed
Substituting values and solving,
ConcepTest
Ready for a Challenge
Sol.
We also know
and
We know
Pause the Video
(Time Duration : 2 Minutes)
11P13.1
CV 2
Pressure Calculation and Kinetic Interpretation of Temperature
Some Definitions :
Root Mean Square Speed :
The RMS value of a set of values is the square root of the arithmetic mean of the squares of the values.
Translational Kinetic Energy of a Gas :
The total translational kinetic energy of all the molecules of the gas will be equal to the summation of kinetic energy of all the molecules.
Calculation of the pressure of an ideal gas :
Ideal Gas
We know,
Pressure by gas on the wall
Change in momentum of one particle in one collision
Time between two collision with wall
Calculation of the pressure of an ideal gas :
Ideal Gas
Total Force by all molecules
Due to symmetry,
Calculation of the pressure of an ideal gas :
For velocity of any particle
Ideal Gas
Calculation of the pressure of an ideal gas :
Ideal Gas
Calculation of the pressure of an ideal gas :
Ideal Gas
Kinetic Interpretation of Temperature :
According to KTG
We know
For 1 mole ideal gas
Constant for a gas
i.e.
Translational Kinetic Energy of a Gas :
The total translational kinetic energy of all the molecules of the gas will be equal to the summation of kinetic energy of all the molecules.
So
The average K.E of a molecule
Translational Kinetic Energy of a Gas :
We know,
For ideal gas
Root Mean Square Speed (RMS Speed) :
The square root of mean square speed is called root-mean-square speed or rms speed.
We know
For ideal gas
Root Mean Square Speed (RMS Speed) :
We know
Root Mean Square Speed (RMS Speed) :
or
Boyle’s Law on the basis of Kinetic theory :
It states that the pressure of a given mass of an ideal gas is inversely proportional to its volume at a constant temperature.
We know
We know for a given gas
i.e. for a given temperature
ConcepTest
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Sol.
Pause the Video
(Time Duration : 2 Minutes)
Q. What will be the change in rms speed of gas on increasing pressure ?
A) Increases
B) Decreases
D) Can’t say
C) Remains constant
We know
We can not comment on speed when pressure is changed.
Answer : C
Explanation :
11P12.3
PSV 1
Sol.
At STP,
We know,
ConcepTest
Ready for a Challenge
Q. Which of the following parameters is the same for molecules of all gases at a given temperature ?
Sol.
Pause the Video
(Time Duration : 2 Minutes)
Answer : D
A) Mass
B) Speed
C) Momentum
D) Kinetic Energy
Explanation :
We know
If temperature is fixed
11P12.3
PSV 2
Sol.
We know,
For same temperature,
For two different gases ,
ConcepTest
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Sol.
Pause the Video
(Time Duration : 2 Minutes)
Answer : C
Explanation : If there is one molecule in the container then all the velocities will be equal.
Summary :
Summary :
Reference Questions
NCERT : 13.1, 13.2, 13.3, 13.7, 13.8, 13.9.
Workbook : 1, 4, 5, 6, 7, 9, 10, 11, 12, 13, 15, 18, 19.
11P13.2
Degree of Freedom and Energy of Gases
Learning Objectives
Degree of Freedom
Law of Equipartition of Energy
Mean Free Path
Specific Heat Capacity of Gases
11P13.2
CV 1
Degree of Freedom and Equipartition Law
Degree of Freedom :
For Translatory Motion :
A particle moving in a straight line along any one of the axes has one degree of freedom.
A particle moving in a plane (X and Y axes) has two degrees of freedom.
A particle moving in space (X, Y and Z axes) has three degrees of freedom.
Simple pendulum
It is defined as the total number of independent variables required to describe the position and configuration of the system.
A point mass can not undergo rotation, but only translatory motion.
A rigid body with finite mass has both rotatory and translatory motion.
The rotatory motion also can have three co-ordinates in space, like translatory motion.
For Rotatory Motion :
Law of Equipartition of Energy :
It states that for a dynamical system in thermal equilibrium, the total energy is equally distributed in all possible energy modes (degree of freedom).
According to kinetic theory of gases,
The mean kinetic energy of a molecule of monoatomic gas
Since molecules move at random,
Law of Equipartition of Energy :
Energy associated with each degree of freedom per molecule
Examples : Molecules of rare gases like helium, argon, etc.
Monoatomic molecule :
Since a monoatomic molecule consists of only a single atom of point mass.
It has three degrees of freedom of translatory motion along the three co-ordinate axes .
Monoatomic molecule :
Internal energy of a monoatomic gas
Hence, a diatomic molecule has five degrees of freedom.
Diatomic molecule :
The diatomic molecule can rotate about any axis at right angles to its own axis.
Hence it has two degrees of freedom of rotational motion in addition to three degrees of freedom of translational motion along the three axes.
Diatomic molecule :
Potential energy of two molecules
Kinetic energy
of vibration
If Diatomic gas molecule have considerable vibration. Then,
Diatomic molecule :
For non-vibrating:
For vibrating:
Triatomic molecule (Linear Type) :
In the case of triatomic molecule of linear type, the center of mass lies at the central atom.
It therefore behaves like a diatomic molecule with three degrees of freedom of translation and two degrees of freedom of rotation, totally it has five degrees of freedom.
Triatomic molecule (Nonlinear Type) :
A triatomic non-linear molecule may rotate, about the three mutually perpendicular axes. Therefore, it possesses three degrees of freedom of rotation in addition to three degrees of freedom of translation along the three co-ordinate axes.
Hence, it has six degrees of freedom.
11P13.2
PSV 1
Answer : D
Sol:
Since the gas is changed to monoatomic gas
11P13.2
CV 2
Specific Heat Capacities of Gases and Mean Free Path
Specific Heat Capacity of Gases :
Monoatomic Gases :
In monoatomic gas, molecules have three translational degrees of freedom.
For one mole of such gas at constant volume,
Internal Energy
Specific Heat Capacity of Gases :
According to the first law of thermodynamics
Where
Specific Heat Capacity of Gases :
If heat transfer takes place at constant volume
Since the volume is constant
For monoatomic gas
By the definition of molar specific heat
Specific Heat Capacity of Gases :
We know from 1st law of thermodynamics
For ideal gas heat transfer at constant pressure
Substituting in 1st law of thermodynamics
Specific Heat Capacity of Gases :
We know
and
Specific Heat Capacity of Gases :
Diatomic Gases :
In case of diatomic gases, there are two possibilities :
i) Molecule is a Rigid Rotator :
In this scenario, the molecule will have five degrees of freedom.
3 Translational
5 Degrees of Freedom
Specific Heat Capacity of Gases :
By the law of equipartition of energy
We know
We know
Internal energy of a molecule of diatomic gas
Internal energy at constant volume
By the definition of molar specific heat
Specific Heat Capacity of Gases :
We know
and
Specific Heat Capacity of Gases :
ii) Molecule is not a Rigid Rotator :
In this scenario, the molecule will have two additional vibrational degree of freedom.
So the internal energy can thus be calculated as
Specific Heat Capacity of Gases :
Internal energy at constant volume
By the definition of molar specific heat
We know
Specific Heat Capacity of Gases :
We know
and
Specific Heat Capacity of Gases :
Polyatomic Gases :
The degrees of freedom of polyatomic gases are,
Deploying the Law of Equipartition of Energy for calculation of internal energy
we get,
Specific Heat Capacity of Gases :
The molar specific heat capacities of polyatomic gases using same analysis done for monoatomic gases.
Specific Heat Capacity of Solids :
Each atom is oscillating along its mean position
Potential energy of two molecules
Kinetic energy
of vibration
Hence, the average energy in three dimensions of the atom would be
For one mole of solid
Specific Heat Capacity of Solids :
In case of solids, volume change is negligible.
From 1st law of thermodynamics
Specific Heat Capacity of Water :
And, following a similar calculation like solids
For the purpose of calculation of specific heat capacity, water is treated as a solid.
A water molecule has three atoms.
Hence, its internal energy would be
11P13.2
PSV 2
A) 22 calorie
B) 4 calorie
C) 8 calorie
D) 12 calorie
Sol:
We know
(For a monoatomic gas)
(For a diatomic gas)
Thus for the mixture
Answer : (B)
Mean Free Path :
Hence, a molecule follows a chain of zigzag paths. Each of these paths is known as a free path which lies between two collisions.
The Kinetic theory of gases assumes that molecules are continuously colliding with each other and they move with constant speeds and in straight lines between two collisions.
Free path
Mean Free Path :
The average of the distances travelled by the molecule between all the collisions is known as Mean Free Path.
The number of collisions increases if the gas is denser or the molecules are large in size.
The mean free path
Summary :
Degree of Freedom defined as the total number of independent variables required to describe the position and configuration of the system.
Law of equipartition of energy states that for a dynamical system in thermal equilibrium, the total energy is equally distributed in all possible energy modes (degree of freedom).
The average of the distances travelled by the molecule between all the collisions is known as Mean Free Path.
Reference Questions
NCERT – 13.4, 13.5 ,13.6, 13.10.
Workbook –2, 3, 8, 14, 16, 17, 20.