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Entropy Change in Entropy Reversible Isobaric Process Ideal Gas in - - PowerPoint PPT Presentation

Entropy Change in Entropy Reversible Isobaric Process Ideal Gas in a Reversible Process Free Expansion of an Ideal Gas Microscopic Interpretation of Entropy Entropy and the Second Law of Thermodynamics


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SLIDE 1

Entropy

  • Change in Entropy
  • Reversible Isobaric Process
  • Ideal Gas in a Reversible Process
  • Free Expansion of an Ideal Gas
  • Microscopic Interpretation of Entropy
  • Entropy and the Second Law of Thermodynamics
  • Homework
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SLIDE 2

Change in Entropy

  • The second law of thermodynamics states that when irreversible (real) processes occur, the disor-

der in the system plus the surroundings increases

  • The measure of disorder in a system is called entropy
  • The change in entropy
✁ ✂
  • f a system as it moves through an infinitesimal process between two

equilibrium states is

✁ ✂ ✄ ✁ ☎ ✆ ✝

where

✁ ☎ ✆

is the heat transferred in a reversible process between the same two states

  • The change in entropy
✞ ✂
  • f a system as it goes from an initial state

to a final state

is

✞ ✂ ✄ ✡ ☛ ☞ ✁ ☎ ✆ ✝
  • Entropy is a state variable like internal energy and temperature
✌ ✁ ✂ ✄ ✍
  • The change in entropy for an irreversible process can be determined by calculating the change in

entropy for a reversible process with the same initial and final states

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SLIDE 3

Example 1

Calculate the change in entropy when 0.235 kg of ice melts at 0

C.

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SLIDE 4

Change in Entropy for a Reversible Isobaric Process

✁ ☎ ✆ ✄ ✏ ✑ ✒ ✁ ✝ ✁ ✂ ✄ ✁ ☎ ✆ ✝ ✄ ✏ ✑ ✓ ✁ ✝ ✝ ✡ ✔ ✕ ✔ ✖ ✁ ✂ ✄ ✏ ✑ ✓ ✡ ✗ ✕ ✗ ✖ ✁ ✝ ✝ ✞ ✂ ✄ ✂ ☛ ✘ ✂ ☞ ✄ ✏ ✑ ✓✚✙ ✛✢✜ ✣ ✝ ☛ ✝ ☞ ✤ ✥
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SLIDE 5

Change in Entropy for a Reversible Process with an Ideal Gas

✁ ✂ ✄ ✁ ☎ ✆ ✝ ✄ ✁ ✦ ☞✧★ ✩ ✪ ✁ ✫ ✝ ✁ ✦ ☞✧ ★ ✄ ✏ ✑ ✬ ✁ ✝ ✪ ✫ ✄ ✏ ✭ ✝ ✁ ✂ ✄ ✏ ✑ ✬ ✁ ✝ ✝ ✩ ✏ ✭ ✁ ✫ ✫ ✡ ✔ ✕ ✔ ✖ ✁ ✂ ✄ ✏ ✑ ✬ ✡ ✗ ✕ ✗ ✖ ✁ ✝ ✝ ✩ ✏ ✭ ✡ ✬ ✕ ✬ ✖ ✁ ✫ ✫ ✞ ✂ ✄ ✂ ☛ ✘ ✂ ☞ ✄ ✏ ✑ ✬ ✙ ✛ ✜ ✣ ✝ ☛ ✝ ☞ ✤ ✥ ✩ ✏ ✭ ✙ ✛ ✜ ✣ ✫ ☛ ✫ ☞ ✤ ✥

Note that it is clear from this result that the change in entropy depends only on the properties of the initial state (

✝ ☞

and

✫ ☞

) and the properties of the final state (

✝ ☛

and

✫ ☛

)

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SLIDE 6

Free Expansion of an Ideal Gas

  • Consider the example of free expansion shown below in which gas that is confined in the left half
  • f an insulated container is allowed to expand into a larger volume
  • The process is irreversible - it does not occur in reverse with the gas spontaneously collecting

itself in the left half of the container

  • The container is insulated, so
✁ ☎ ✄ ✍
  • The walls are rigid, so
✁ ✮ ✄ ✘ ✪ ✁ ✫ ✄ ✍
  • From the first law of thermo we have
✁ ✦ ☞✧★ ✄ ✍

, so

✝ ☞ ✄ ✝ ☛
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SLIDE 7

Free Expansion of an Ideal Gas (cont’d)

  • To calculate the change in entropy for free expansion, we need to consider a reversible process

that connects the same initial and final states

  • We can use the isothermal expansion of an ideal gas
✁ ☎ ✆ ✄ ✘ ✁ ✮ ✄ ✪ ✁ ✫ ✄ ✏ ✭ ✝ ✁ ✫ ✫ ✁ ✂ ✄ ✁ ☎ ✆ ✝ ✄ ✏ ✭ ✁ ✫ ✫ ✡ ✔ ✕ ✔ ✖ ✁ ✂ ✄ ✏ ✭ ✡ ✬ ✕ ✬ ✖ ✁ ✫ ✫ ✞ ✂ ✄ ✂ ☛ ✘ ✂ ☞ ✄ ✏ ✭ ✙ ✛✢✜ ✣ ✫ ☛ ✫ ☞ ✤ ✥✰✯ ✍
  • Example 2: One mole of nitrogen undergoes free expansion to double its volume. What is the

change in entropy of the gas?

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SLIDE 8

Microscopic Interpretation of Entropy

  • Consider the free expansion of an ideal gas
  • If we assume that each molecule occupies a volume
✫ ✱

and that each location of a molecule is equally probable, then the total number of possible locations, or microstates, in the initial volume

✫ ☞

is

✲ ☞ ✄ ✫ ☞ ✳ ✫ ✱
  • The number of possible microstates for

molecules in the initial volume is

✮ ☞ ✄ ✲✶✵ ☞ ✄ ✷ ✫ ☞ ✳ ✫ ✱ ✸ ✵
  • Similarly, the number of possible microstates for

molecules in the final volume is

✮ ☛ ✄ ✲ ✵ ☛ ✄ ✷ ✫ ☛ ✳ ✫ ✱ ✸ ✵
  • The probability
  • f a given macrostate is proportional to the number of microstates correspond-

ing to the macrostate, and thus the ratio of the probabilities of given initial and final macrostates

  • ccurring is
✪ ☛ ✪ ☞ ✄ ✮ ☛ ✮ ☞ ✄✺✹ ✬ ✕ ✬ ✻ ✼ ✵ ✽ ✬ ✖ ✬ ✻ ✾ ✵ ✄ ✜ ✣ ✫ ☛ ✫ ☞ ✤ ✥ ✵
  • Taking the natural log and multiplying by Boltzmann’s constant we have
✿ ❀ ✙ ✛ ✜ ✣ ✮ ☛ ✮ ☞ ✤ ✥ ✄ ✏ ✴ ❁ ✿ ❀ ✙ ✛❂✜ ✣ ✫ ☛ ✫ ☞ ✤ ✥ ✿ ❀ ✙ ✛ ✮ ☛ ✘ ✿ ❀ ✙ ✛ ✮ ☞ ✄ ✏ ✭ ✙ ✛ ✜ ✣ ✫ ☛ ✫ ☞ ✤ ✥
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SLIDE 9

Microscopic Interpretation of Entropy (cont’d)

  • Earlier we found that the change in entropy for free expansion of an ideal gas in terms of the

macroscopic thermodynamic variables is

✂ ☛ ✘ ✂ ☞ ✄ ✏ ✭ ✙ ✛ ✜ ✣ ✫ ☛ ✫ ☞ ✤ ✥
  • Comparison of the previous two expressions yields the following connection between entropy and

the number of microstates associated with a given macrostate

✂ ❃ ✿ ❀ ✙ ✛ ✮
  • This is the famous Boltzmann’s entropy equation, and is engraved on his tombstone
  • Example 3: One mole of nitrogen undergoes free expansion to double its volume. Use the micro-

scopic interpretation of entropy to find the change in entropy of the gas?

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SLIDE 10

Entropy and The Second Law of Thermodynamics

  • The second law of thermo can be stated in terms of entropy as: The entropy of an isolated system

never decreases. It can only stay the same or increase.

✞ ✂ ❄ ✍ ✷ ✟❅❆ ❇❈❉❊ ✁ ❅ ❋ ❅ ❉❊
  • If the system is not isolated, then the change in entropy of the system plus the change in entropy
  • f the environment must be greater than or equal to zero
✞ ✂ ✄ ✞ ✂ ❍ ✩ ✞ ✂ ■ ✧❏ ❄ ✍
  • Only (idealized) reversible, cyclic processes have
✞ ✂ ✄ ✍
  • The total entropy of any system plus that of its environment increases as a result of any natural

process

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SLIDE 11

Homework Set 9 - Due Fri. Jan. 30

  • Read Sections 18.6 - 18.8
  • Answer Questions 18.8 & 18.11
  • Do Problems 18.22, 18.23, 18.26, 18.28 & 18.33