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Packet 3.4 Thermodynamics

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Thermodynamics Internal Energy W = P V 1st Law of Thermodynamics: U = Q W Define: Adiabatic, isothermal, isobaric & isochoric and show these on a P-V diagram – PowerPoint PPT presentation

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Title: Packet 3.4 Thermodynamics


1
Packet 3.4Thermodynamics
  • Internal Energy
  • W P?V
  • 1st Law of Thermodynamics ?U Q W
  • Define Adiabatic, isothermal, isobaric
    isochoric and show these on a P-V diagram
  • Irreversibility disorder
  • Entropy is a measure of disorder
  • State 2nd Law of Thermodynamics
  • Heat engine efficiency, ? W/Qh
  • Carnot Engine
  • Energy Degradation

2
Internal Energy
  • Is the total potential and kinetic energy of the
    molecules in a substance.
  • Potential energy is associated with
    intermolecular forces.
  • Kinetic energy includes both translational and
    rotational motion.
  • When we consider an ideal gas, the intermolecular
    forces are assumed to be zero!
  • Internal energy of a gas comes only from the
    random kinetic energy of the atom of the gas.

3
Ideal Gas Internal Energy
  • Ek 1/2mv2 3/2kT so, U 3/2 NkT
  • U 3/2nRT
  • ? U 3/2 nR ? T

4
Ideal Gas Internal Energy
  • What is the internal energy of 30 moles of oxygen
    gas at room temperature?
  • U 3/2nRT

5
Ideal Gas Internal Energy
  • If the room were moving at a high velocity would
    that mean the internal energy of the gas would be
    greater?

6
Work done on or by a gas
  • Imagine compressing a gas by exerting a force on
    the piston from the outside.
  • Consider heating the piston and it expands to
    perform work.
  • W F x D F PA
  • W P (A x D)
  • W P ? V

7
Example
  • A gas is compressed at constant pressure 2.00 x
    105 Pa from a volume of 2.00 m3 to a volume of
    0.500 m3.
  • What is the work done on the gas.
  • If the temperature initially was 40 C what is
    the final temperature of the gas?

8
Thermodynamic Processes
  • CLICK HERE TO GO OVER EACH PROCESS!!

Isochoric Isobaric
Isothermal
Const. Volume Const. Pressure
Const. Temp
  • Remember! Area under curve is Work Done!

9
Adiabatic Expansion
  • Rapid expansion or compression of a gas.
  • No Heat (Q) can flow in or out of the system. ?Q
    0
  • Any work done equals a direct change in internal
    energy. ?U ?W
  • Bottle Rockets
  • Diesel Engines

10
Figure 18-11Adiabatic Heating
11
The First Law of Thermodynamics (FLT)
-- Heat and work are forms of energy transfer and
energy is conserved.
?U Q - Wby
change in total internal energy
work done by the system
heat added to system
State Function Process Functions
or ?U Q Won
12
"Process Problems"
For which process is W the largest?
smallest?For which process is Q the largest?
smallest?
13
Physics Joke
  • Once all the scientists die and go to heaven.
    They decide to play hide-n-seek and Einstein goes
    first. Einstein counts up to 100 and then start
    searching. Everyone starts hiding except Newton.
    Newton just draws a square of 1 meter and stands
    in it, right in front of Einstein. Einsteins
    counting ....97,98,99,100, opens his eyes and
    finds Newton standing in front. Einstein says
    "Newtons out, Newtons out." Newton denies and
    says I am not out. He claims that he is not
    Newton. All the scientists come out and he proves
    that he is not Newton. How??

14
His proof
  • Newton says I am standing in a square of area 1m
    square.. That means I am Newton per meter
    square.. Hence I am Pascal. Since newton per
    meter square Pascal

15
Conceptual Checkpoint 18-2Which is the adiabatic
curve?
16
The second law of thermodynamics
  • When objects of different temperatures are
    brought into thermal contact, the spontaneous
    flow of heat that results is always from the high
    temperature object to the low temperature object.

17
Heat Engines
  • Energy goes in
  • Useful Work taken out
  • Some gets wasted
  • Max Efficiency TH Tc/ Th x 100

18
The 2nd Law of Thermodynamics
  • The second law of thermodynamics deals with the
    limitations imposed on heat engines that is on
    devices whose aim is to covert heat (disordered
    energy) into mechanical energy (ordered energy).

19
The 2nd Law of Thermodynamics
  • The Entropy of an isolated system never
    decreases.
  • It is impossible for heat to (spontaneously) flow
    from a cold to a hot object.
  • It is impossible for a heat engine working in a
    cycle to absorb heat and perform an equal amount
    of work.
  • The most efficient heat engine operating between
    two given temperatures is the Carnot Engine.

20
Entropy
  • Entropy like Internal energy is a State Function!
  • Entropy Is a measure of the disorder of a system.
  • ?S ?Q/T
  • If ?Q gt 0 entropy increases
  • If ?Q lt 0 entropy decreases.

21
Philosophy
  • Three Laws of Thermodynamics (paraphrased) First
    Law You can't get anything without working for
    it. Second Law The most you can accomplish by
    work is to break even. Third Law You can't break
    even.
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