Reversible and irreversible processes Physics 110 -- Entropy 28 - - PowerPoint PPT Presentation

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Reversible and irreversible processes Physics 110 -- Entropy 28 - - PowerPoint PPT Presentation

Reversible and irreversible processes Physics 110 -- Entropy 28 September 2011 Isolated systems thermal reservoir may exchange heat temperature does not change battery reversibly stores work engine may exchange heat or work


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SLIDE 1

Reversible and irreversible processes

Physics 110 -- Entropy 28 September 2011

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SLIDE 2

Isolated systems

thermal reservoir

  • may exchange heat
  • temperature does not change

battery

  • reversibly stores work

engine

  • may exchange heat or work
  • operates in a cycle

ideal gas

  • may exchange heat or work
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SLIDE 3

Heat flow

Second Law of Thermodynamics (Clausius) No process can have as its sole result the transfer

  • f heat from a colder system to a warmer system.

warmer

q

colder warmer

q

colder possible impossible

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SLIDE 4

Heat flow

warmer

q

colder warmer

q

colder irreversible same

q

same reversible possible possible impossible Second Law of Thermodynamics (Clausius) No process can have as its sole result the transfer

  • f heat from a colder system to a warmer system.
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SLIDE 5

Work and heat

????

q w

q = w

q w

q = w possible

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SLIDE 6

Work and heat

q w q

warmer colder q = w Overall process violates the Second Law! possible impossible

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SLIDE 7

Work and heat

q w q w

q = w q = w possible impossible irreversible

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SLIDE 8

Expansion of an ideal gas

Q = 0 W = 0 ∆E = 0 ∆T = 0

q w

isothermal expansion

∆E = 0 q = w We can also perform isothermal compression.

free expansion possible possible reversible

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SLIDE 9

Free compression?

???? free compression

Q = 0 W = 0 ∆E = 0 ∆T = 0

warmer

q

colder

w q Step 1: isothermal expansion Note that the gas has expanded.

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SLIDE 10

free compression

Q = 0 W = 0 ∆E = 0 ∆T = 0

warmer

Step 2: free compression

colder

Overall process violates the Second Law! impossible

Free compression?

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SLIDE 11

Expansion of an ideal gas

q w

free expansion isothermal expansion

Q = 0 W = 0 ∆E = 0 ∆T = 0 ∆E = 0 q = w We can also perform isothermal compression.

reversible possible possible irreversible

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SLIDE 12

Heat engines

perfect heat engine

q w

impossible

warmer

q w

colder

q' q-q'=w

general heat engine possible*

*provided waste heat q' is not too small

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SLIDE 13

Refrigerators

impossible possible*

*provided work input w is not too small

perfect refrigerator

q

warmer colder

q w q=w+q'

general refrigerator

q'

warmer colder

q

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SLIDE 14

End review