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Thermodynamics
Heat and Work
•Heat can be used to do work.
•Energy transferred to heat
turns water into steam which
then exerts a force on a
turbine and does work.
Work Equation
•Work = Pressure x volume
change
•W = P x ∆V
•Volume = Area x distance
(cylinder)
•Work is in Joules (J)
Isovolumetric Process
• No work is done if the volume is
not changed (to have work you
must have movement)
• When a gas undergoes a change in
temperature but no change in
volume, no work is done. This is
an isovolumetric process.
Isothermal Process
• When the system’s temperature
remains constant and the internal
energy does not change when energy
is transferred to or from the system as
heat or work it is called an isothermal
process.
• Pressure can change but not
temperature.
Adiabatic Process
• A thermodynamic process during
which work is done but no energy is
transferred as heat.
• Q = 0
• No heat can be lost because there is
usually not enough time in the
process. (It happens to quickly for
heat to escape)
1st Law of Thermodynamics
•The principle of energy
conservation that takes into
account a system’s internal
energy as well as work and
heat is called the first law of
thermodynamics.
1st Law Equation
• ∆U = Q – W
• The Q and W can be positive or negative
depending on circumstances.
• If the Q is negative and the W is positive,
just insert that into the above equation:
• ∆U = -Q –W and you would get a
negative number or your answer.
Signs for Q and W
• Q = + if energy is added to the system
as heat.
• Q = - if energy is removed from the
system as heat.
• W = + if work is done by the system
• W = - if work is done on the system
Cyclic Process
• A thermodynamic process in which a
system returns to the same conditions
under which it started is called a cyclic
process.
• For example, a refrigerator energy is
transferred in four steps. However, the
process restarts each time under the same
conditions. - no loss or gain of energy
Heat Engines
• Heat engines use heat to do work.
• Equation to measure amount of work:
• Work net = Heat transferred from the
heat engine – Heat taken by other
object
• Wnet = Qh - Qc
Gas Engine - Steps
• Step 1: Spark plug fires.
• Step 2: Gas is ignited.
• Step 3: Gas creates pressure.
• Step 4: Pressure moves Piston.
• Step 5: Piston moves crankshaft.
2nd Law of Thermodynamics
• No cyclic process that converts
heat entirely into work is possible.
• In other words, some energy must
always be transferred as heat to the
environment.
• Cannot be 100% efficient!
Efficiency Equation
•Eff = Wnet / Qh
•Eff = (Qh – Qc)/Qh
•Eff = 1 – (Qc/Qh)
Entropy
• Entropy is the measure of a
system’s disorder.
• In general, it is believed that
without interference, disorder is
more likely than order.
• The greater the system’s disorder,
the greater the system’s entropy.
• Greater disorder or entropy means
there is less energy to do work.
• Imagine atoms in an engine
bouncing around chaotically
compared to atoms all bouncing
(pushing) in the same direction.
The ordered atoms will accomplish
more work.
THE END OF THE UNIVERSE!
• Since everything in the world is moving towards
chaos, it has been suggested that eventually the
entire world will reach a maximum value of entropy
(chaos).
• At that time, the universe will reach a state of
thermal equilibrium and the temperature will be the
same everywhere.
• Since there will be no temp difference, no heat can
be transferred and thus no work can be done.
• This is called ultimate “heat death” of the universe
and is predicted to happen in 100 trillion years. So
make your plans now!
Thermodynamics

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Thermodynamics

  • 2. Heat and Work •Heat can be used to do work. •Energy transferred to heat turns water into steam which then exerts a force on a turbine and does work.
  • 3. Work Equation •Work = Pressure x volume change •W = P x ∆V •Volume = Area x distance (cylinder) •Work is in Joules (J)
  • 4. Isovolumetric Process • No work is done if the volume is not changed (to have work you must have movement) • When a gas undergoes a change in temperature but no change in volume, no work is done. This is an isovolumetric process.
  • 5. Isothermal Process • When the system’s temperature remains constant and the internal energy does not change when energy is transferred to or from the system as heat or work it is called an isothermal process. • Pressure can change but not temperature.
  • 6. Adiabatic Process • A thermodynamic process during which work is done but no energy is transferred as heat. • Q = 0 • No heat can be lost because there is usually not enough time in the process. (It happens to quickly for heat to escape)
  • 7. 1st Law of Thermodynamics •The principle of energy conservation that takes into account a system’s internal energy as well as work and heat is called the first law of thermodynamics.
  • 8. 1st Law Equation • ∆U = Q – W • The Q and W can be positive or negative depending on circumstances. • If the Q is negative and the W is positive, just insert that into the above equation: • ∆U = -Q –W and you would get a negative number or your answer.
  • 9. Signs for Q and W • Q = + if energy is added to the system as heat. • Q = - if energy is removed from the system as heat. • W = + if work is done by the system • W = - if work is done on the system
  • 10. Cyclic Process • A thermodynamic process in which a system returns to the same conditions under which it started is called a cyclic process. • For example, a refrigerator energy is transferred in four steps. However, the process restarts each time under the same conditions. - no loss or gain of energy
  • 11. Heat Engines • Heat engines use heat to do work. • Equation to measure amount of work: • Work net = Heat transferred from the heat engine – Heat taken by other object • Wnet = Qh - Qc
  • 12. Gas Engine - Steps • Step 1: Spark plug fires. • Step 2: Gas is ignited. • Step 3: Gas creates pressure. • Step 4: Pressure moves Piston. • Step 5: Piston moves crankshaft.
  • 13. 2nd Law of Thermodynamics • No cyclic process that converts heat entirely into work is possible. • In other words, some energy must always be transferred as heat to the environment. • Cannot be 100% efficient!
  • 14. Efficiency Equation •Eff = Wnet / Qh •Eff = (Qh – Qc)/Qh •Eff = 1 – (Qc/Qh)
  • 15. Entropy • Entropy is the measure of a system’s disorder. • In general, it is believed that without interference, disorder is more likely than order. • The greater the system’s disorder, the greater the system’s entropy.
  • 16. • Greater disorder or entropy means there is less energy to do work. • Imagine atoms in an engine bouncing around chaotically compared to atoms all bouncing (pushing) in the same direction. The ordered atoms will accomplish more work.
  • 17. THE END OF THE UNIVERSE! • Since everything in the world is moving towards chaos, it has been suggested that eventually the entire world will reach a maximum value of entropy (chaos). • At that time, the universe will reach a state of thermal equilibrium and the temperature will be the same everywhere. • Since there will be no temp difference, no heat can be transferred and thus no work can be done. • This is called ultimate “heat death” of the universe and is predicted to happen in 100 trillion years. So make your plans now!