Entropy Second Law of Thermodynamics PHYS116 A02 4182013

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Entropy, Second Law of Thermodynamics PHYS-116 A-02 4/18/2013 Lecture 24 Momchil Velkovsky

Entropy, Second Law of Thermodynamics PHYS-116 A-02 4/18/2013 Lecture 24 Momchil Velkovsky

Example, Diatomic Gas: 700 J of heat is transferred to a diatomic gas, while

Example, Diatomic Gas: 700 J of heat is transferred to a diatomic gas, while keeping the pressure constant. The temperature during the process is such that the rotational dof are unfrozen, but the vibrational ones are frozen. How much of the heat goes towards changing the internal energy and how much towards work? What part of the internal energy is translational KE, and what part rotational KE?

The Adiabatic Expansion of an Ideal Gas, Q=0

The Adiabatic Expansion of an Ideal Gas, Q=0

A Diesel engine has a compression ratio of 20: 1 What is the final

A Diesel engine has a compression ratio of 20: 1 What is the final temperature in the cylinder?

Heat transfer mechanisms • Heat conduction • Heat convection • Thermal Radiation

Heat transfer mechanisms • Heat conduction • Heat convection • Thermal Radiation

Conduction of heat II • This is a good reason not to pick up

Conduction of heat II • This is a good reason not to pick up a metal frying pan by its bare handle. • ks=50. 2 W/(m K), kc=385 W/(m K)

Convection of heat • Heating by moving large amounts of hot fluid, usually water

Convection of heat • Heating by moving large amounts of hot fluid, usually water or air. • Viscosity causes a surface film (equivalent to 1. 3 cm of plywood) • P~(TH-TC)5/4

Radiation of heat • Infrared lights, hot metal objects, a fireplace, standing near a

Radiation of heat • Infrared lights, hot metal objects, a fireplace, standing near a running furnace … these are all objects heating others by broadcast of EM radiation just lower in energy than visible red. • P=Aes. T 4 , -8 W/(m 2 K 4) s=5. 6 x 10

Microscopic states Tossing a coin helps to picture the outcomes of a statistic event.

Microscopic states Tossing a coin helps to picture the outcomes of a statistic event. To model atoms or molecules, we need ~1023 “coins” with many possible outcomes (not just “heads” or “tails”).

http: //vimeo. com/1224449 Entropy

http: //vimeo. com/1224449 Entropy

Statistical model of a gas

Statistical model of a gas

Directions for thermodynamic processes The maximum useful outcome will come from a reversible process

Directions for thermodynamic processes The maximum useful outcome will come from a reversible process (like taking a building apart piece by piece) instead of an irreversible process (like imploding the same building with explosives). Nature favors disorder over order. (It is hard to build a tower, but easier to knock it down with explosives. )

Entropy for different processes What is the change of the entropy for an adiabatic

Entropy for different processes What is the change of the entropy for an adiabatic process? What is the change of the entropy for an reversible isothermal process?

Heath engines As heat flows from a reservoir at higher temperature to a sink

Heath engines As heat flows from a reservoir at higher temperature to a sink at lower temperature, work may be removed.

Heath engines and the Second Law of Thermodynamics

Heath engines and the Second Law of Thermodynamics

Perfect (Carnot) Engine Refrigirator

Perfect (Carnot) Engine Refrigirator

Carnot Engine

Carnot Engine

Thermodynamic cycles

Thermodynamic cycles