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Thermodynamics

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Thermodynamics The study of heat energy through random systems Laws of Thermodynamics 0th Law: If Ta=Tb and Tb=Tc then Ta=Tc 1st Law: E=W+Q (Conservation of Energy ... – PowerPoint PPT presentation

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Title: Thermodynamics


1
Thermodynamics
  • The study of heat energy
  • through random systems

2
Laws of Thermodynamics
  • 0th Law If TaTb and TbTc then TaTc
  • 1st Law ?EWQ (Conservation of Energy)
  • The increase in thermal energy of a system is
    determined by the heat of the system and the work
    added to it.
  • The idea behind the Heat Engine

3
Efficiency
  • WnetQnetQhot-Qcold
  • or EffWnet/Qhot1-(Qcold/Qhot)
  • Ex A steam engine absorbs 1.98 x105J and expels
    1.49 x105J in each cycle. Assume that all the
    remaining energy is used to do work.
  • a. What is the engines efficiency?
  • b. How much work is done in each cycle?

4
  • a. Eff0.247
  • b. W4.9 x104J

5
  • 2nd Law A system can be defined by its entropy.
    In a closed system entropy tends to increase.
  • Entropy A measure of the disorder (randomness)
    of the system
  • 3rd Law Temperature and Entropy are absolute
    scales.
  • At some point no temperature or entropy exists.
  • T?0 K and S?S0

6
Heat Engines
  • Engines allow heat energy to be transformed into
    work or mechanical energy.
  • Work or Energy ?Heat increases
  • no big deal. Friction does this.
  • Heat ?Work or Energy
  • is a big deal. Heat is easy to move around. You
    could just bring heat wherever you needed work
    done and Boom! you wouldnt have to do the
    work, a machine could.
  • Work or Energy ?Heat decreases
  • is also a big deal. Making food cold preserves
    it and allows it to be moved readily. Less
    spoilage means less disease.

7
  • Any heat engine works on the same properties.
  • A hot reservoir is the source of the energy.
  • Both words mean something. Hot means that there
    is plenty of heat energy and reservoir means that
    if heat is removed the temperature doesnt drop
    much.
  • There is also a need for a cold reservoir.
    Again, both words mean something.
  • Cold because it is at a lower temperature than
    the hot reservoir and reservoir because it must
    be large enough that you can dump heat into it
    without appreciably raising the temperature.

8
What happens if we put a hot and cold reservoir
in contact? Thermal Equilibrium is not the
answer!
  • Heat transfer (or flow) is the answer.
  • Remember that these are reservoirs so it would
    take a long time for them to come into thermal
    equilibrium.
  • This is great, but we dont get any work out of
    it.
  • We need to steal some of the energy leaving the
    hot reservoir and make it do work for us.

9
Heat Engine
  • Stealing some energy to do work

10
Types of Heat Engine
  • Steam Engine

11
Internal Combustion Engine
12
Unfortunately we dont get an even trade!
  • We lose energy to randomness/Entropy
  • This is the 2nd Law of Thermodynamics
  • Automobile engines are only about 15 efficient.
    That means for every 100J of heat energy, 15J
    worth of work is done on the piston and 85J of
    heat are discarded. Still, this is the source of
    energy for most of our transportation.

13

14
  • If a steam engine takes in 2.254 x 104 kJ of heat
    and gives up 1.915 x 104 kJ of heat to the
    exhaust, what is the engines efficiency?

15
We can go backwards!
  • This is a refrigerator or air conditioner

W
16
This requires Energy/Work
  • This is why your refrigerator must be plugged in.
  • It is constantly dumping heat into your kitchen
  • Due to the 2nd Law of Thermodynamics more heat is
    dumped than is removed
  • If you left the refrigerator door open you would
    heat up the kitchen

17
Perfect Heat Engine
18
(No Transcript)
19
Efficiency
  • WnetQnetQhot-Qcold
  • or EffWnet/Qhot(1-Qcold/Qhot)
  • Ex A steam engine absorbs 1.98 x105J and expels
    1.49 x105J in each cycle. Assume that all the
    remaining energy is used to do work.
  • a. What is the engines efficiency?
  • b. How much work is done in each cycle?

20
  • a. Eff0.247
  • b. W4.9 x104J

21
More 2nd Law
  • Entropy
  • Sentropy
  • QHeat (Joules)
  • TTemperature (In Kelvin)
  • Entropy in a system must increase or at least
    stay the same!!!!!!!!!!!!

22
  • An engine has a hot reservoir at 1000 K and uses
    the atmosphere at 300 K as the cold reservoir.
    You take 2500 J from the hot reservoir to do 1900
    J of work.
  • A. How much heat goes into the atmosphere?
  • B. Is this engine possible? (Does the entropy
    increase?)

23
  • WnetQnetQhot-QcoldQcoldQhot-Wnet2500J -1900J
    600J
  • EntropyEngine is not possible.
  • What is the maximum amount of work we can take
    out?
  • How much work is done?

24
Carnot Engine
  • Maximum efficiency
  • In theory could run backwards
  • All temperatures in Kelvin
  • What is the efficiency of an ideal steam engine
    with steam at 685 K and exhaust at 298 K?
  • What is Qcold ?

25
Carnot Engine
  • Maximum efficiency
  • In theory could run backwards
  • All temperatures in Kelvin
  • What is the efficiency of an ideal steam engine
    with steam at 685 K and exhaust at 298 K?
  • What is Qhot if Qcold is 450J?
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