Chapter 4 (Volume 2) - Second Law of Thermodynamics · Second Law of Thermodynamics Entropy Engines...

Chapter 4 (Volume 2) -Second Law of

Thermodynamics

Entropy

Engines

Refrigerators

Statistics of Entropy

Chapter 4 - Second Law of Thermodynamics

“The motive power of heat is independent of the agentsemployed to realize it.”

-Nicolas Léonard Sadi Carnot

David J. StarlingPenn State Hazleton

Fall 2013

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

An irreversible process is a process that cannot

occur spontaneously in the opposite direction.

Examples:

I the warming of your hands by a hot cup of tea;

I the breaking of a glass;

I the hatching of an egg.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

An irreversible process is a process that cannot

occur spontaneously in the opposite direction.

Examples:

I the warming of your hands by a hot cup of tea;

I the breaking of a glass;

I the hatching of an egg.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

What makes these processes irreversible? It’s not

the energy—energy is still conserved!

The order of the object has changed. The object is moredisordered.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

What makes these processes irreversible? It’s not

the energy—energy is still conserved!

The order of the object has changed. The object is moredisordered.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

The disorder of system is a state property, just like

pressure and temperature, that depends only on

the current state and not how it got there.

The measure of disorder is known as entropy.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

The disorder of system is a state property, just like

pressure and temperature, that depends only on

the current state and not how it got there.

The measure of disorder is known as entropy.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

The definition of the change in entropy of a closed

system from one state to another is:

∆S = Sf − Si =

And remember: it doesn’t matter how the system gets fromone state the next.

I For a reversible process: ∆S = 0

I For an irreversible process: ∆S > 0

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

∆S = Sf − Si =

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

∆S = Sf − Si =

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

To calculate the change in entropy of a closed

system, sometimes we can play a trick.

Calculate the integral for the reversible process—it’s mucheasier!

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

To calculate the change in entropy of a closed

system, sometimes we can play a trick.

Calculate the integral for the reversible process—it’s mucheasier!

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

Consider the same initial and final volumes and moles, witha constant temperature. Then,

∆S =

(isothermal process)

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

Consider the same initial and final volumes and moles, witha constant temperature. Then,

∆S =

(isothermal process)

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

In a closed system, the entropy always increases

for an irreversible process, and remains the same

for a reversible process.

∆S ≥ 0 (2)

This is the Second Law of Thermodynamics.Entropy always increases or stays the same in any process.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

∆S ≥ 0 (2)

This is the Second Law of Thermodynamics.

Entropy always increases or stays the same in any process.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

∆S ≥ 0 (2)

This is the Second Law of Thermodynamics.Entropy always increases or stays the same in any process.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy

A box with five adiabatic sides contains an ideal gas with aninitial temperature T0. The sixth side is placed in contactwith a reservoir with a constant temperature T2 > T0. Whymust the entropy change of the universe always beincreasing as the box warms?(a) Entropy will always be increasing since the work done

on the gas in the box is negative.(b) Entropy will always be increasing since the

temperature of the box is always ≤ T2.(c) Entropy will always be increasing since this process is

reversible.(d) Entropy will always be increasing since the

temperature of the box is always greater than absolutezero.

(e) Entropy will always be increasing since in any processentropy increases.

Thermodynamics

Entropy

Engines

Refrigerators

Engines

An engine is a device that extracts heat from the

environment and converts it to work.

I Every engine needs a working substance (water/steam,

air, gasoline)

I The working substance moves in a cycle composed of

strokes

Thermodynamics

Entropy

Engines

Refrigerators

Engines

An engine is a device that extracts heat from the

environment and converts it to work.

I Every engine needs a working substance (water/steam,

air, gasoline)

I The working substance moves in a cycle composed of

strokes

Thermodynamics

Entropy

Engines

Refrigerators

Engines

How much work W can be done with a given

amount of heat QH?

I An ideal engine is one that does not suffer from waste

(friction, turbulence).

I A perfect engine is one that converts 100% of its heat

to work.

Is this possible?

Thermodynamics

Entropy

Engines

Refrigerators

Engines

amount of heat QH?

to work.

Is this possible?

Thermodynamics

Entropy

Engines

Refrigerators

Engines

amount of heat QH?

to work.

Is this possible?

Thermodynamics

Entropy

Engines

Refrigerators

Engines

Let’s look at the Carnot engine and compute its

efficiency.

I Heat is absorbed by the working substanceI Some energy is converted to work, some is dumped as

Thermodynamics

Entropy

Engines

Refrigerators

Engines

efficiency.

Thermodynamics

Entropy

Engines

Refrigerators

Engines

efficiency.

Thermodynamics

Entropy

Engines

Refrigerators

Engines

The efficiency of an engine can be calculated:

ε =energy we get

energy we pay for=|W||QH|

=|QH| − |QL||QH|

= 1− |QL||QH|

I Measuring the heat transfer can be tricky

I Let’s analyze the cycle and try to compute this ratio

Thermodynamics

Entropy

Engines

Refrigerators

Engines

ε =energy we get

=|QH| − |QL||QH|

= 1− |QL||QH|

Thermodynamics

Entropy

Engines

Refrigerators

Engines

ε =energy we get

=|QH| − |QL||QH|

= 1− |QL||QH|

Thermodynamics

Entropy

Engines

Refrigerators

Engines

Compute the change in entropy for a full cycle:

∆S = ∆Sa→b + ∆Sb→c + ∆Sc→d + ∆Sd→a

= ∆SH + ∆SL

=|QH|TH− |QL|

|QL||QH|

Thermodynamics

Entropy

Engines

Refrigerators

Engines

∆S = ∆Sa→b + ∆Sb→c + ∆Sc→d + ∆Sd→a

= ∆SH + ∆SL

=|QH|TH− |QL|

|QL||QH|

Thermodynamics

Entropy

Engines

Refrigerators

Engines

∆S = ∆Sa→b + ∆Sb→c + ∆Sc→d + ∆Sd→a

= ∆SH + ∆SL

=|QH|TH− |QL|

= 0|QL||QH|

Thermodynamics

Entropy

Engines

Refrigerators

Engines

∆S = ∆Sa→b + ∆Sb→c + ∆Sc→d + ∆Sd→a

= ∆SH + ∆SL

=|QH|TH− |QL|

|QL||QH|

Thermodynamics

Entropy

Engines

Refrigerators

Engines

∆S = ∆Sa→b + ∆Sb→c + ∆Sc→d + ∆Sd→a

= ∆SH + ∆SL

=|QH|TH− |QL|

|QL||QH|

Thermodynamics

Entropy

Engines

Refrigerators

Engines

The efficiency of the Carnot engine depends only

on the temperatures of the hot and cold reservoirs.

ε = 1− TL

Thermodynamics

Entropy

Engines

Refrigerators

Engines

The Carnot engine is an ideal engine in that its

efficiency is as high as possible.

I Isothermal expansion and

compression (constant T)

I Adiabatic expansion and

compression (Q = 0)

Thermodynamics

Entropy

Engines

Refrigerators

Engines

The Carnot engine is an ideal engine in that its

efficiency is as high as possible.

I Isothermal expansion and

compression (constant T)

I Adiabatic expansion and

compression (Q = 0)

Thermodynamics

Entropy

Engines

Refrigerators

Engines

The Stirling engine has lower efficiency but is

more practical.

I Isothermal expansion and compression (constant T)

I Constant volume heating/cooling (Q 6= 0)

Thermodynamics

Entropy

Engines

Refrigerators

Engines

The Stirling engine has lower efficiency but is

more practical.

I Isothermal expansion and compression (constant T)

I Constant volume heating/cooling (Q 6= 0)

Thermodynamics

Entropy

Engines

Refrigerators

Engines

During the power stroke of an internal combustion engine,the air-fuel mixture is ignited and the expanding hot gasespush on the piston. Assuming the engine exhibits thehighest efficiency possible, which of the followingstatements concerning the exhaust gas must be true to avoidviolating the second law of thermodynamics?(a) The exhaust gas must be hotter than the outside air

temperature.(b) The exhaust gas must be at the same pressure as the

outside air.(c) The exhaust gas must be cooled to the same

temperature as the outside air.(d) The exhaust gas must be cooled below the temperature

of the outside air.(e) Real engines will always violate the second law of

thermodynamics.

Thermodynamics

Entropy

Engines

Refrigerators

Engines

Consider the various paths shown on the pressure-volumegraph. By following which of these paths, does the systemdo the most work?

(a) 1 to 2 to 4

(b) 1 to 4

(c) 1 to 3 to 4

(d) Each of these paths results in the same amount of workdone.

Thermodynamics

Entropy

Engines

Refrigerators

An ideal refrigerator operates in reverse of an

engine.

We put in work which draws heat from the cold reservoirand dumps it into the hot reservoir.

Thermodynamics

Entropy

Engines

Refrigerators

An ideal refrigerator operates in reverse of an

engine.

We put in work which draws heat from the cold reservoirand dumps it into the hot reservoir.

Thermodynamics

Entropy

Engines

Refrigerators

The coefficient of performance is defined in a

similar way as before:

K =what we want

what we pay for=|QL||W|

|QH| − |QL|

We can simplify this further by using |QL||QH | = TL

TH − TL

Thermodynamics

Entropy

Engines

Refrigerators

K =what we want

|QH| − |QL|

TH − TL

Thermodynamics

Entropy

Engines

Refrigerators

K =what we want

|QH| − |QL|

TH − TL

Thermodynamics

Entropy

Engines

Refrigerators

You are repairing a window-style air conditioner in a closedworkroom. You succeed in getting it to work, but are calledaway soon after you turn it on. Unfortunately, you areunable to return for several hours to turn it off. Assumingthat it was running as efficiently as possible while you wereaway, how has the temperature of the workroom changed inyour absence?

(a) The room is somewhat cooler than before I left.

(b) The room is slightly cooler than before I left.

(c) The temperature of the room has not changed.

(d) The room is warmer than before I left.

(e) The air near the ceiling will be very warm, but the airaround the air conditioner will be very cool.

Thermodynamics

Entropy

Engines

Refrigerators

Entropy can be calculated by considering the

possible arrangements of atoms/molecules in a

given system.

If we have six molecules in a box, what are their possiblecombinations?

Thermodynamics

Entropy

Engines

Refrigerators

Entropy can be calculated by considering the

possible arrangements of atoms/molecules in a

given system.

If we have six molecules in a box, what are their possiblecombinations?

Thermodynamics

Entropy

Engines

Refrigerators

In mathematics, the number of combinations of N

things taken k at a time can be computed as:

k!(N − k)!(4)

For example: given three fruit (apple, orange, banana), how

many combinations of two can be made?

I apple + orange, apple + banana, orange + banana = 3

)= 3!/[2!(3− 2)!] = 3× 2× 1/(2× 1× 1) = 3.

Thermodynamics

Entropy

Engines

Refrigerators

k!(N − k)!(4)

)= 3!/[2!(3− 2)!] = 3× 2× 1/(2× 1× 1) = 3.

Thermodynamics

Entropy

Engines

Refrigerators

k!(N − k)!(4)

)= 3!/[2!(3− 2)!] = 3× 2× 1/(2× 1× 1) = 3.

Thermodynamics

Entropy

Engines

Refrigerators

Given a box of 6 particles, how many

configurations are there if we split them left/right?

Seven: 6-0, 5-1, 4-2, 3-3, 2-4, 1-5, 0-6.Each of these configurations can be done in one or moreways.

Thermodynamics

Entropy

Engines

Refrigerators

Seven: 6-0, 5-1, 4-2, 3-3, 2-4, 1-5, 0-6.

Each of these configurations can be done in one or moreways.

Thermodynamics

Entropy

Engines

Refrigerators

Seven: 6-0, 5-1, 4-2, 3-3, 2-4, 1-5, 0-6.Each of these configurations can be done in one or moreways.

Thermodynamics

Entropy

Engines

Refrigerators

For the configuration shown (4-2), how many

combinations are there?

I W =(6

)= 6!/2!4! = 6× 5/2 = 15

I W is called the multiplicity of the 4-2 configuration.

I Each of the 15 combinations is called a microstate

I The configuration (4-2) is known as the macrostate

Thermodynamics

Entropy

Engines

Refrigerators

I W =(6

)= 6!/2!4! = 6× 5/2 = 15

Thermodynamics

Entropy

Engines

Refrigerators

I W =(6

)= 6!/2!4! = 6× 5/2 = 15

Thermodynamics

Entropy

Engines

Refrigerators

I W =(6

)= 6!/2!4! = 6× 5/2 = 15

Thermodynamics

Entropy

Engines

Refrigerators

I W =(6

)= 6!/2!4! = 6× 5/2 = 15

Thermodynamics

Entropy

Engines

Refrigerators

We can list a number of important features:

I The more evenly distributed the configuration, the

higher the multiplicity.

I The more microstates for a configuration, the more

likely that configuration.

I The lower the multiplicity, the lower the entropy

I The higher the multiplicity, the higher the entropy

Thermodynamics

Entropy

Engines

Refrigerators

We can list a number of important features:

I The more evenly distributed the configuration, the

higher the multiplicity.

I The more microstates for a configuration, the more

likely that configuration.

I The lower the multiplicity, the lower the entropy

I The higher the multiplicity, the higher the entropy

Thermodynamics

Entropy

Engines

Refrigerators

To obtain the entropy of a system, we use the

famous Boltzmann entropy equation:

S = k ln W (5)

with k = 1.381× 10−23 J/K the Boltzmann constant.

Thermodynamics

Entropy

Engines

Refrigerators

If the multiplicity is very large, we can compute S

with Stirling’s approximation,

ln N! ≈ N ln N − N. (6)

(different Stirling from the engine guy)

Thermodynamics

Entropy

Engines

Refrigerators

In the system shown,

(a) the number on a die corresponds to a microstate, andthe numbers on all the dice (1, 2, 4, 6) correspond tothe macrostate;

(b) the number on a die corresponds to a microstate, andthe sum of the numbers on all the dice corresponds tothe macrostate;

(c) the numbers on all the dice correspond to a microstate,and the sum of the numbers on all the dice correspondsto the macrostate;

(d) the sum of the numbers on all the dice corresponds to amicrostate, and the numbers on all the dice correspondto the macrostate.

Chapter 4 (Volume 2) - Second Law of Thermodynamics · Second Law of Thermodynamics Entropy Engines...

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