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KTG & THERMODYNAMICS

JEE MAIN CHAPTER OVERVIEW

Chapter Priority

1 (HIGHEST)

Number of problems in PYQ

HIGH

Difficulty

Easy

KEY CONCEPTS FOR JEE MAIN

Thermodynamics is a branch of Physics that deals with the conversion of heat into other forms of energy.


POSTULATES OF KTG

· Gases are made up of large number identical molecules

· Size of molecules is very small as compared to the distance between them

· Molecules undergo elastic collisions

· Force between molecules is negligible except during collision

· As a whole, molecules are moving randomly, i.e., they move in all directions with equal probability and with speeds varying from very low to very high values


IMPLICATIONS OF POSTULATES

· Volume of the molecules is negligible as compared to volume of the container

· Molecules can have varying speeds – very low, medium or very high.

· Proportion of molecules with a given speed does not change even after collisions. (This means that we can draw a graph of speed on x-axis and % of molecules on y-axis and this graph remains the same as time passes)

· Potential energy between molecules is ZERO as there is no force between them except during collision.


MEAN FREE PATH

Mean free path is the average distance a molecule can travel between two successive collisions.

Mean Free Path of molecule in a gas
Random Path & Collision of a Molecule in a Gas

Mean free path (lambda) is give by:


Mean Free Path of a molecule in a gas. Kinetic Theory Of Gases. IIT JEE PHYSICS. JEE MAIN

Using PV = nRT, Mean Free Path can also be written as


Mean Free Path of a molecule in terms of Pressure and Temperature.

From the above we can conclude that, mean free path is proportional to ratio of (T/P)

TRY JEE MAIN PYQ

The mean free path of molecules of a certain gas at STP is 1500d, where d is the diameter of the gas molecules. While maintaining the standard pressure, the mean free path of the molecules at 373 K is approximately :


[Hint: Mean free path is proportional to ratio T/P]


[If you cannot solve any question, upload a photo of your doubt at www.savai.co.in or WhatsApp me @ 7982286138, we will send solution.]


VELOCITIES OF MOLECULES

We define three special velocities of a gas under Kinetic Theory.


When,

M0 = Molecular mass of the gas

T = Temperature of the gas


Average velocity of gas molecules is given by

Average velocity of gas molecules in kinetic theory of gases

RMS Velocity of gas molecules is given by

RMS Velocity of gas molecules in Kinetic Theory of Gases

Most probable Velocity

Most probable velocity of gas molecules

Note: VMP < VAVG < VRMS

[This is often asked directly in JEE MAIN]


Pressure & RMS Velocity

Relation between Pressure and Vrms of a gas is given by:

Pressure and RMS velocity of a gas

MAXWELL'S DISTRIBUTION CURVE

[Not important for JEE MAIN but it is good to know where the above velocities were derived from]


Within a volume, gas molecules will have all possible speeds ranging from ZERO to infinity. The fraction of gas molecules with a given speed is the Maxwell distribution curve.


The x-axis represents the speed of molecules and the y-axis represents the Maxwell Distribution Function.


[Again, not important for JEE but technically, the fraction of molecules having speeds in the range dv is equal to the area of the shaded rectangle, Nvdv. The function Nv approaches zero as v approaches infinity. ]


Vmp, Vavg and Vrms are derived from this function.

Maxwell's distribution curve for speed of molecules of a gas. Kinetic Theory of Gases. IIT JEE.

TRY JEE MAIN PYQ:

Q. The temperature of an ideal gas is increased from 200 K to 800 K. If r.m.s. speed of gas at 200 K is V0. Then, r.m.s. speed of the gas in terms of V0 at 800 K will be?


[Hint: Vrms is proportional to square root of T]


Q. The rms speed of oxygen molecule in a vessel at particular temperature is

[(1 + 5/x)^0.5]*v

where is the average speed of the molecule. The value of x will be:

(Take pie = 22/7)


[Hint: Write down the formula for both Vrms and Vavg and use the above equation as well]

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MOLAR SPECIFIC HEAT


Molar specific heat is the heat energy required to raise the temperature of one mole of a substance by 1 degree celsius. It is represented by 'C'

Molar Specific Heat and SI Unit of Molar Specific Heat

We can also write:

dQ = nC(dT)


For gases, always remember, C depends upon the process.

Cadiabatic = 0 [No heat is transferred in adiabatic process]

Cisothermal = infinity [Temperature does not change in isothermal process]


For isobaric (constant pressure) process, Cp is given by:

Molar specific heat at constant pressure

For isochoric (constant volume) process, Cv is given by:

molar specific heat at constant volume

Other important formulae:

CP - CV = R


Ratio of Cp/Cv is called (gamma)

Gamma (Ratio of molar specific heat at constant pressure and volume)

We can also write

DEGREE OF FREEDOM (f)

It represents the number of independent ways a gas molecule can move.

A molecule can either

  1. Translate (Move in a straight line in x/y/z direction)

  2. Rotate (Spin about an axis in x/y/z direction)

  3. Vibrate (Move back and forth in x/y/z direction)

Not all molecules will have the ability rotate or vibrate across all (x/y/z) axis.


Depending upon the structure of the molecule, degrees of freedom (f) are calculated.


Remember, Cp and Cv are dependent on degrees of freedom:


Cv = f(R/2)


Cp = R + f(R/2)


Cp/Cv = 1 + (2/f)


Vibrational modes of freedom are not a part of JEE Syllabus


Given below are the degrees of freedom (f), Cp , Cv and Cp/Cv values for various molecular structures

[Note:Vibrational modes of freedom are not a part of JEE Syllabus]

Gas

f

Cv

Cp

Cp/Cv

Monoatomic

3

3R/2

5R/2

5/3

Diatomic

5

5R/2

7R/2

7/5

Linear Triatomic

5

5R/2

7R/2

7/5

Triatomic

6

3R

4R

4/3

MIXTURE OF GASES

Let there be a mixture of two gases.

Let (n1, Cp, Cv) be the number of moles & molar specific heats of Gas 1

Let (n2,Cp2,Cv2) be the number of moles & molar specific heats of Gas 2


Equivalent Molar Specific heat at constant pressure is

Equivalent Molar Specific heat at constant pressure of a mixture of gases


Equivalent Molar Specific heat at constant Volume is

Equivalent Molar Specific heat at constant volume of a mixture of gases

Equivalent Gamma(Cp/Cv)

Equivalent gamma for a mixture of gases (Cp/Cv). Kinetic Theory of gases. IIT JEE MAIN.


INTERNAL ENERGY OF A GAS


Energy associated with a gas due to its Temperature. It is represented by 'U'


It represents the Kinetic Energy of a gas which is a result of Temperature alone.


[Note: Remember, within internal energy there is no component of potential energy because we assume there is no force between molecules.]


Internal Energy (U) is given by:

U = nCv(T)

dU = nCv(dT)

Where, Cv is the molar specific heat at constant volume. T is the temperature.


dT>0 => dU increases

dT<0 => dU decreases


Remember, this U is solely a function of T. The above formula is true under any process (isochoric, isobaric, isothermal, adiabatic etc.).


Law of Equipartition of Energy

Each degree of freedom has equal kinetic energy (kT/2) associated with it.


k = Boltzmann Constant = (R/NA)

Boltzmann Constant

For example,


A monoatomic gas has 3 degrees of freedom. Thus,


Energy of each molecule = (3kT/2)

Energy of a mole (U) = (3kT/2)*NA = (3R/2)*T

Energy of 'n' moles = n*(3R/2)*T = n*(Cv)*T


[Note: Cv (monoatomic) = 3R/2]


For any gas,

Internal energy Ugas = (f/2)*nRT

TRY A JEE MAIN PYQ

Q. The temperature at which the kinetic energy of oxygen molecules becomes double than its value at 27°C is?


[Hint: Use Kelvin scale for temperature & Kinetic energy is internal energy dependent on Temperature alone. Oxygen is diatomic so use approriate Cv.]

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Q. A gas mixture consists of 2 moles of oxygen and 4 moles of neon at temperature T. Neglecting all vibrational modes, the total internal energy of the system will be?

[Hint: U(total) = U(O2) + U(He)]


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WORK DONE BY A GAS

When a gas expands the work done by gas (W) = P(dV)

Work done by a gas in expansion

dV = Change in volume

W>0 when dV>0 [when gas expands]

W<0 when dV<0 [when gas compressed]


W = Area under P-V curve

Work done is are under PV graph

FIRST LAW OF THERMODYNAMICS

The form of the first law useful for JEE MAIN is -


"Heat Given to System leads to Change in Internal Energy of Gas and Work Done by the Gas"

First law of thermodynamics

It can also be written for small change in Q,W or U. Remember the following formulae:


dQ = dW + dU


dU = nCv(dT)


dW = P(dV)


dQ = nCdT


dU is always nCv(dT) irrespective of process. Cv is the molar specific at constant volume.

dQ is by definition nC(dT). Here C is the molar specific heat of the process involved.

dQ>0

Heat supplied to the system

dQ<0

Heat taken from the system

dU>0

temperature of gas increases

du<0

temperature of gas decreases

dW>0

Volume of gas increases

dW<0

Volume of gas decreases

ISOBARIC PROCESS

Pressure = Constant


PV = nRT


W = P(V2 - V1)


In isobaric process, Volume is proportional to to temperature

In isobaric process, Volume is proportional to Temperature

P-V graph is a straight line parallel to x-axis

In isobaric process, PV curve is a straight line

ISOCHORIC PROCESS

Volume = Constant

PV = nRT

W = 0 (ZERO)


In Isochoric process, Pressure is proportional to temperature


Pressure proportional to temperature in constant volume

PV curve is a straight line perpendicular to x-axis.

PV curve is vertical in constant volume process

ISOTHERMAL PROCESS

Temperature = Constant

PV = nRT

PV = Constant

P1V1 = P2V2

In isothermal process, PV is constant

Work done in isothermal process:

Work done in isothermal process

P-V graph of Isothermal Process

Pressure-Volume graph of isothermal process is a hyperbola

Since, Temperature is constant, internal energy (U) is constant.

dU = 0

dQ = dW

Heat supplied = Work done by Gas


ADIABATIC PROCESS

dQ = 0

No heat is exchanged in this process

dQ = 0

dU + dW = 0

dW = -dU

dU = nCv(dT)

dW = -nCv(dT)


Relation between Pressure and Volume in Adiabatic Process

Relation between Pressure and Volume in adiabatic process

Pressure-Volume graph slopes downwards

Pressure-Volume graph slopes downwards in adiabatic process

Relation between Temperature and Volume

Relation between temperature and volume in adiabatic process

Graph of temperature-volume in adiabatic process slopes downwards

Temperature-volume graph in adiabatic process

Relation between Pressure and Temperature in adiabatic process

Relation between Pressure and Temperature in adiabatic process

Graph of pressure and temperature in adiabatic process slopes upwards

graph of pressure and temperature of adiabatic process

Work done in adiabatic process

dW = -dU

dW = -nCv(dT)

Now, Cv can be written as:

Molar specific heat at constant volume, R and gamma

Work done in adiabatic process:

Work done in adiabatic process

Comparison P-V graphs of adiabatic and isothermal:

CYCLIC PROCESS

Processes in which gas starts and ends at the same state are called cyclic processes.


The P-V graph of a cyclic process forms a closed loop.


Work done in cyclic process = Area of the loop

if process clockwise, W>0 (positive)

if process anti-clockwise, W<0 (negative)


GAS UNDER FREE EXPANSION

When gas expands against a vacuum, Pressure of the gas is Zero.

Therefore Work done by gas = ZERO

Free expansion of gas against vacuum

TRY JEE MAIN PYQ

Q. A source supplies heat to a system at the rate of 1000 W. If the system performs work at a rate of 200 W. The rate at which internal energy of the system increase is?


[Hint: Write first law of thermodynamics and divide equation by time to get rate.]


[If you cannot solve any question, upload a photo of your doubt at www.savai.co.in or WhatsApp me @ 7982286138, we will send solution.]


Q. The Thermodynamic process, in which internal energy of the system remains constant is?

[If you cannot solve any question, upload a photo of your doubt at www.savai.co.in or WhatsApp me @ 7982286138, we will send solution.]



SUMMARY OF PROCESSES

PROCESS

PROPERTY

ISOTHERMAL

Internal energy is constant. Heat supplied to gas equals work done by gas.

ISOBARIC

The heat absorbed goes partly to increase internal energy and partly to do work

ISOCHORIC

No work is done on or by the gas

ADIABATIC

Work done by the gas decreases internal energy

POLYTROPIC PROCESSES

Processes whose P-V curve is of the form:

For example:

Molar specific heat of a polytropic process is given by:


MIXING TWO GASES

This topic is learnt from an example:


Case 1: Same gas in two containers:

Same gas having characteristics P1, V1,T1 & P2, V2, T2 is placed in two chambers as shown. Find final temperature & pressure of mixture if knob is removed. Assume no heat is loss from the container.


dQ = 0

dW = 0 [since total volume remains constant, work done by system is ZERO]

Therefore, dU = 0 [from 1st Law of Thermodynamics]


Get n1 and n2 from PV = nRT


Equate initial internal energy and final internal energy

Case 2: Different gas in two containers:

Different gases having characteristics P1, V1,T1 & P2, V2, T2 is placed in two chambers as shown. Find final temperature & pressure of mixture if knob is removed. Assume no heat is loss from the container.


dQ = 0

dW = 0 [since total volume remains constant, work done by system is ZERO]

Therefore, dU = 0 [from 1st Law of Thermodynamics]

Get n1 and n2 from PV = nRT


Equate initial internal energy and final internal energy

Keep in mind, Use Cv_equivalent in the above equation:



SECOND LAW OF THERMODYNAMICS

KEVIN-PLANCK STATEMENT

"It is impossible to construct a heat engine which can give 100% efficiency"


HEAT ENGINES

Heat engine converts heat into mechanical energy.


For example, when you boil water in a kettle and keep a lid on top, after a while the pressure from steam causes the lid to move a little. Heat from burning of gas is converted into motion of lid.


In a heat engine there are three parts:

  1. Source: This part provides the heat energy to the system. This is at a high temperature (T1).

  2. Working Substance: This is the gas which will do Work.

  3. Sink: This is the part to which residual heat is lost. It is at a low temperature (T2).


In the above boiling water example, the burning of cooking gas provides heat (it is the source), steam/water is the working substance and air around the kettle is the sink.



Q1: Heat supplied by source

W: Work done by working substance

Q2: Heat rejected to sink

(These represent magnitudes only, take signs accordingly)


From 1st law:

Q1 = W + Q2


Efficiency = (Work Done/Heat Supplied)*100


CARNOT CYCLE

Carnot cyle is the most efficient heat engine. It represent a cyclic process with 4 stages:


Stage 1: Isothermal Expansion (AB)

Stage 2: Adiabatic Expansion (BC)

Stage 3: Isothermal Compression (CD)

Stage 4: Adiabatic Compression (DA)


Carnot Cycle

Assume:

A (P1,V1), B (P2,V2), C (P3,V3), D (P4,V4)

A & B have same Temperature (T1)

C & D have same Temperature (T2)


The following equations hold true for Carnot cycle:


V2*V4 = V1*V3

For a Carnot cycle, from the above volume relation we can derive the following:

Efficiency of Carnot engine can be written as:

TRY A JEE MAIN PYQ:

Work done by a Carnot engine operating between temperatures 127°C and 27°C is 2 kJ. The amount of heat transferred to the engine by the reservoir is?


[Hint: Write Temperature in Kelvin]

[If you cannot solve any question, upload a photo of your doubt at www.savai.co.in or WhatsApp me @ 7982286138, we will send solution.]


A carnot engine with efficiency 50% takes heat from a source at 600K. In order to increase the efficiency to 70%, keeping the temperature of sink same, the new temperature of the source will be?


[Hint: Write efficiency formula in terms Temperature]

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2nd Law of Thermodynamics


Clausius Statement:

"It is impossible to Construct a Refrigerator unaided by any external agent, which would transfer heat from a body at a low Temperature to Another Body at a High Temperature."


Refrigerator takes heat from a cold body and throws away this heat to a hot body. For example, the refrigerator in your home would take heat from inside (where temperature is low) and throw that heat into the atmosphere (where temperature is high)


The refrigerator takes heat Q2 from sink with the help of work W done by external agent and throws out heat Q1 to the atmosphere.


We define a coefficient of performance

Entropy

It is the degree of randomness of a system


It is represented by S.


Change in entropy equals the (Heat supplied to the system/Temperature)

Change in entropy: dS = dQ/T

dQ = T(dS)

[This can be used in dQ = dW + dU]


Area under T-S curve gives us the heat supplied to a system (integral of TdS).


Hope you can REVISE KTG & THERMODYNAMICS FOR JEE MAIN PHYSICS from this guide to answer all varieties of JEE MAIN PYQs. Thanks a lot!


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