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The kinetic theory of gases

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Course of lectures «Contemporary Physics: Part1»Lecture №8The Kinetic Theory of Gases.Heat Engines, Entropy, and the Second Law of Thermodynamics.

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Слайд 1Quick Quiz 4.1 Suppose you are standing directly behind someone

who steps back and accidentally stomps on your foot with

the heel of one shoe. Would you be better off if that person were (a) a large professional basketball player wearing sneakers (b) a petite woman wearing spike-heeled shoes?

Quick Quiz 4.2 A grandfather clock depends on the period of a pendulum to keep correct time. Suppose a grandfather clock is calibrated correctly and then a mischievous child slides the bob of the pendulum downward on the oscillating rod. Does the grandfather clock run (a) slow (b) fast (c) correctly?

Quick Quiz 4.1 Suppose you are standing directly behind someone who steps back and accidentally stomps on

Слайд 2Course of lectures «Contemporary Physics: Part1»
Lecture №8

The Kinetic Theory of

Gases.
Heat Engines, Entropy, and the Second Law of Thermodynamics.

Course of lectures «Contemporary Physics: Part1»Lecture №8The Kinetic Theory of Gases.Heat Engines, Entropy, and the Second Law

Слайд 3Molecular Model of an Ideal Gas
The macroscopic description of model

of ideal gas make the following assumptions:

1. The number of

molecules in the gas is large, and the average separation between them is large compared with their dimensions.
2. The molecules obey Newton’s laws of motion, but as a whole they move randomly.
3. The molecules interact only by short-range forces during elastic collisions.
4. The molecules make elastic collisions with the walls.
5. The gas under consideration is a pure substance; that is, all molecules are identical.
Molecular Model of an Ideal GasThe macroscopic description of model of ideal gas make the following assumptions:1.

Слайд 4Molecular Model of an Ideal Gas

Molecular Model of an Ideal Gas

Слайд 5Molecular Model of an Ideal Gas

Molecular Model of an Ideal Gas

Слайд 6Molecular Model of an Ideal Gas
(10.1)

Molecular Model of an Ideal Gas(10.1)

Слайд 7Molecular Model of an Ideal Gas

Molecular Model of an Ideal Gas

Слайд 8Molecular Model of an Ideal Gas
(10.2)
The pressure of a gas

is proportional to the number of molecules per unit volume

and to the average translational kinetic energy of the molecules,
Molecular Model of an Ideal Gas(10.2)The pressure of a gas is proportional to the number of molecules

Слайд 9Molecular Interpretation of Temperature
This result tells us that temperature is

a direct measure of average molecular kinetic energy.
(10.3)
(10.4)
(10.5)

Molecular Interpretation of TemperatureThis result tells us that temperature is a direct measure of average molecular kinetic

Слайд 10Molecular Interpretation of Temperature
Theorem of equipartition of energy
each degree of

freedom contributes ½kbT to the energy of a system, where

possible degrees of freedom in addition to those associated with translation arise from rotation and vibration of molecules.

(10.7)

(10.6)

Molecular Interpretation of TemperatureTheorem of equipartition of energyeach degree of freedom contributes ½kbT to the energy of

Слайд 11Molecular Interpretation of Temperature
Table 10.1

Molecular Interpretation of TemperatureTable 10.1

Слайд 12Molar Specific Heat of an Ideal Gas
molar specific heats:
(10.8)
(10.9)
(10.10)

Molar Specific Heat of an Ideal Gasmolar specific heats:(10.8)(10.9)(10.10)

Слайд 13Molar Specific Heat of an Ideal Gas
If energy is transferred

by heat to a system at constant volume, then no

work is done on the system. From the first law of thermodynamics, we see that

(10.11)

(10.12)

(10.13)

(10.14)

Molar Specific Heat of an Ideal GasIf energy is transferred by heat to a system at constant

Слайд 14Molar Specific Heat of an Ideal Gas
(10.15)

Molar Specific Heat of an Ideal Gas(10.15)

Слайд 15Molar Specific Heat of an Ideal Gas
(10.16)
(10.17)

Molar Specific Heat of an Ideal Gas(10.16)(10.17)

Слайд 16Adiabatic Processes for an Ideal Gas
An adiabatic process is one

in which no energy is transferred by heat between a

system and its surroundings.

(10.18)

Home work:

Adiabatic Processes for an Ideal GasAn adiabatic process is one in which no energy is transferred by

Слайд 17The Boltzmann Distribution Law
(10.7)
The number density
(10.19)
The Boltzmann distribution law, is

important in describing the statistical mechanics of a large number

of molecules. It states that the probability of finding the molecules in a particular energy state varies exponentially as the negative of the energy divided by kBT.
The Boltzmann Distribution Law(10.7)The number density(10.19)The Boltzmann distribution law, is important in describing the statistical mechanics of

Слайд 18Distribution of Molecular Speeds
(10.20)

Distribution of Molecular Speeds(10.20)

Слайд 19Distribution of Molecular Speeds

Distribution of Molecular Speeds

Слайд 20Mean Free Path
The average distance between collisions is called the

mean free path.

Mean Free PathThe average distance between collisions is called the mean free path.

Слайд 21Mean Free Path

Mean Free Path

Слайд 22Mean Free Path
(10.21)
(10.22)
Collision frequency f, is

Mean Free Path(10.21)(10.22)Collision frequency f, is

Слайд 23Heat Engines and the Second Law
of Thermodynamics
A heat engine is

a device that takes in energy by heat and, operating

in a cyclic process, expels a fraction of that energy by means of work.

The net work Weng done by a heat engine is equal to the net energy Qnet transferred to it.

Heat Engines and the Second Lawof ThermodynamicsA heat engine is a device that takes in energy by

Слайд 24Heat Engines and the Second Law
of Thermodynamics
The net work done

in a cyclic process is the area enclosed by the

curve representing the process on a PV diagram.

(10.23)

The thermal efficiency

(10.24)

Heat Engines and the Second Lawof ThermodynamicsThe net work done in a cyclic process is the area

Слайд 25On the basis of the fact that efficiencies of real

engines are well below 100%, the Kelvin–Planck form of the

second law of thermodynamics states the following:

Heat Engines and the Second Law
of Thermodynamics

It is impossible to construct a heat engine that, operating in a cycle, produces no effect other than the input of energy by heat from a reservoir and the performance of an equal amount of work.

On the basis of the fact that efficiencies of real engines are well below 100%, the Kelvin–Planck

Слайд 26Heat Pumps and Refrigerators

Heat Pumps and Refrigerators

Слайд 27Heat Pumps and Refrigerators
The Clausius statement states:
It is impossible to

construct a cyclical machine whose sole effect is to transfer

energy continuously by heat from one object to another object at a higher temperature without the input of energy by work.

In simpler terms, energy does not transfer spontaneously by heat from a cold object to a hot object.

The effectiveness of a heat pump is described in terms of a number called the coefficient of performance (COP).

(10.25)

(10.26)

Heat Pumps and RefrigeratorsThe Clausius statement states:It is impossible to construct a cyclical machine whose sole effect

Слайд 28Reversible and Irreversible Processes
In a reversible process, the system undergoing

the process can be returned to its initial conditions along

the same path on a PV diagram, and every point along this path is an equilibrium state. A process that does not satisfy these requirements is irreversible.
Reversible and Irreversible ProcessesIn a reversible process, the system undergoing the process can be returned to its

Слайд 29The Carnot Engine
French engineer named Sadi Carnot showed that a

heat engine operating in an ideal, reversible cycle— called a

Carnot cycle—between two energy reservoirs is the most efficient engine possible.

Carnot’s theorem can be stated as follows:

No real heat engine operating between two energy reservoirs can be more efficient than a Carnot engine operating between the same two reservoirs.

The Carnot EngineFrench engineer named Sadi Carnot showed that a heat engine operating in an ideal, reversible

Слайд 31The Carnot Engine
This result indicates that all Carnot engines operating

between the same two temperatures have the same efficiency.
Hence, the

thermal efficiency of a Carnot engine is

(10.27)

The Carnot EngineThis result indicates that all Carnot engines operating between the same two temperatures have the

Слайд 32Entropy
Isolated systems tend toward disorder and that entropy is a

measure of this disorder.
We distinguish between microstates and macrostates of

a system. A microstate is a particular configuration of the individual constituents of the system.
Macrostate is a description of the conditions of the system from a macroscopic point of view and makes use of macroscopic variables such as pressure, density, and temperature for gases.

Because entropy is a measure of disorder, an alternative way of stating this is the entropy of the Universe increases in all real processes.

EntropyIsolated systems tend toward disorder and that entropy is a measure of this disorder.We distinguish between microstates

Слайд 33Entropy
The change in entropy during a process depends only on

the end points and therefore is independent of the actual

path followed. Consequently, the entropy change for an irreversible process can be determined by calculating the entropy change for a reversible process that connects the same initial and final states.

(10.28)

(10.29)

EntropyThe change in entropy during a process depends only on the end points and therefore is independent

Слайд 34Entropy
Let us consider the changes in entropy that occur in

a Carnot heat engine that operates between the temperatures Tc

and Th. In one cycle, the engine takes in energy Qh from the hot reservoir and expels energy Qc to the cold reservoir.

(10.30)

EntropyLet us consider the changes in entropy that occur in a Carnot heat engine that operates between

Слайд 35Quick Quiz 5.3

If you are asked to make a

very sensitive glass thermometer, which of the following working liquids

would you choose? (a) mercury (b) alcohol (c) gasoline (d) glycerin
Quick Quiz 5.3 If you are asked to make a very sensitive glass thermometer, which of the

Слайд 36Quick Quiz 5.4

Two spheres are made of the same

metal and have the same radius, but one is hollow

and the other is solid. The spheres are taken through the same temperature increase. Which sphere expands more? (a) solid sphere (b) hollow sphere (c) They expand by the same amount. (d) not enough information to say
Quick Quiz 5.4 Two spheres are made of the same metal and have the same radius, but

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