chapter 24 thermodynamics

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Chapter 24 Thermodynami cs

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Chapter 24 Thermodynamics. The study of heat and its transformation into mechanical work. If we increase the thermal motion of atoms what happens? Temperature increases. There seems to be no upper limit of temperature. However, there is a lower limit. Absolute Zero. - PowerPoint PPT Presentation

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Page 1: Chapter 24  Thermodynamics

Chapter 24 Thermodynamics

Page 2: Chapter 24  Thermodynamics

•The study of heat and its transformation into mechanical work.

Page 3: Chapter 24  Thermodynamics

•If we increase the thermal motion of atoms what happens?

Temperature increases.

Page 4: Chapter 24  Thermodynamics

There seems to be no upper limit of temperature.

However, there is a lower limit.

Page 5: Chapter 24  Thermodynamics

Absolute Zero•The point at which all molecular motion stops.

Page 6: Chapter 24  Thermodynamics

•No more energy can be extracted from a substance and the temperature can not be lowered any further.

Page 7: Chapter 24  Thermodynamics

•Kelvin: 0 K

•Celsius: -273 oC

•Fahrenheit: -459 oF

Page 8: Chapter 24  Thermodynamics
Page 9: Chapter 24  Thermodynamics

First Law of Thermodynamics

:The internal energy of an isolated system is

constant.

Page 10: Chapter 24  Thermodynamics

The increase in the internal energy of a system is equal to the amount of energy added by heating the system, minus the amount lost as a result of the work done by the system on its surroundings.

Page 11: Chapter 24  Thermodynamics

Signs (+/-) will tell you if energy is entering or

leaving a system.+ indicates energy enters a system

.- indicates energy leaves a system.

Page 12: Chapter 24  Thermodynamics

First Law of Thermodynamics

                            

             

thermo:     heat       dynamics:  force------------------------------------------------------Work done on water by paddle-wheelis converted to thermal energy.------------------------------------------------------First Law:

Heat added = Work done

                   or

Heat added = Thermal energy increase                                     +                   = Work done by system

Page 13: Chapter 24  Thermodynamics

•Heat can be used to do work.

•Heat and work are energy transferred to or from a system.

Page 14: Chapter 24  Thermodynamics

•Work done on or by a gas is the pressure times the change in volume.

W = PV

Page 15: Chapter 24  Thermodynamics

Work is the transfer of energy that takes place when an object is moved against an opposing force

i.e. a system does work when it expands against an external pressure

Car engine: petrol burns & produces gases which push out pistons in the engine and transfer energy to the

wheels of car

•Work stimulates uniform motion

• Heat and work can be considered as energy in transit

Page 16: Chapter 24  Thermodynamics

Ex: An engine cylinder compresses a volume of gas by 0.04 m3. How much work is done by the cylinder if it exerts a constant pressure of 7.5 x 105 Pa?

Page 17: Chapter 24  Thermodynamics

G: P = 7.5 x 105 Pa, V = 4 x 10-2 m3

U: W = ?

E: W = PV

S: W =(7.5 x 105)(4 x 10-2)

S: W = 30,000 J

Page 18: Chapter 24  Thermodynamics

U = Q + W

• Q = quantity of heat that enters or leaves a system.

Page 19: Chapter 24  Thermodynamics

U = the change in internal energy.

W = work done on (+) or by the system (-).

Page 20: Chapter 24  Thermodynamics

Ex: When 5000 J of heat is added to an engine, the

engine does 1250 J of work. What is the change in the internal energy of

engine?

Page 21: Chapter 24  Thermodynamics

Q = 5000 J

W = 1250 J

U = ?

Page 22: Chapter 24  Thermodynamics

U = Q + W

U = Q – W

U = 5000 J–1250 J

U = 3750 J

Page 23: Chapter 24  Thermodynamics

Adiabatic•The process of compression or expansion of a gas so that no heat enters or leaves a system.

Page 24: Chapter 24  Thermodynamics

•Read Ch 24.3 in CP book.

•Examples combustion engine, bike pump, weather conditions.

Page 26: Chapter 24  Thermodynamics

1. intake/induction stroke

2. compression stroke

3. power stroke4. exhaust stroke

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2nd Law of Thermodynamics

Heat flows spontaneously from a body of a higher

temperature to a one at a lower temperature.

Page 35: Chapter 24  Thermodynamics

Heat EngineAny device that changes internal

energy into mechanical work.

Page 36: Chapter 24  Thermodynamics
Page 37: Chapter 24  Thermodynamics

To reverse the flow work must be done.

Page 38: Chapter 24  Thermodynamics

•Ex: steam engine, internal combustion engine, jet engine, etc.

Page 39: Chapter 24  Thermodynamics

•The basic idea of a heat engine is that mechanical work can be obtained only when heat flows from hot to cold temperatures.

Page 40: Chapter 24  Thermodynamics

•Not all heat is transformed into work.

Page 41: Chapter 24  Thermodynamics

• "Typical engines are only 15 to 20 percent efficient in consuming oil, as they lose a lot of energy when they emit hot exhaust gas into the air."

Page 42: Chapter 24  Thermodynamics

Every heat engine will:

1.Absorb internal energy from a reservoir of higher temperature.

Page 43: Chapter 24  Thermodynamics

2. Convert some of this energy into mechanical work.

3. Expel the remaining energy to some lower temperature reservoir, usually called a “sink”.

Page 44: Chapter 24  Thermodynamics

•When undesirable heat is expelled, its called thermal pollution.

Page 45: Chapter 24  Thermodynamics
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Power plants and industrial factories are among the major contributors to the problem of thermal pollution. These facilities draw water from nearby lakes and streams, which they use to cool their machinery and steam-driven equipment. Although many such facilities now take care not to contaminate the water with chemical pollutants, few return the heated water to its original temperature before dumping it back into the lakes and streams from which it came. The heated water warms local bodies of water by as much as 10° C (18° F), making the water uninhabitable for fish and other organisms.

Page 47: Chapter 24  Thermodynamics

Carnot EfficiencyThe maximum amount of energy that can be converted to work in a heat engine.

Page 48: Chapter 24  Thermodynamics

•This gives us the ‘ideal efficiency’.

Page 49: Chapter 24  Thermodynamics

•This gives us the ‘ideal efficiency’.

hot

coldhot

T

TTeffideal

Page 50: Chapter 24  Thermodynamics

h

ch

Q

QQeff

Page 51: Chapter 24  Thermodynamics
Page 52: Chapter 24  Thermodynamics

Qh = energy added as heat

Qc = energy removed as heat

Page 53: Chapter 24  Thermodynamics

3rd Law of Thermodynamics

There is no process by which a body may be

cooled to a temperature of 0 K (Absolute Zero).

Page 54: Chapter 24  Thermodynamics

Entropy•The measure of the amount of disorder.