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Thermodynamics Thermodynamics

Thermodynamics - PowerPoint Presentation

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Thermodynamics - PPT Presentation

1 st law of thermodynamics Energy may be converted to different forms but it is neither created nor destroyed during transformations Energy from chemical bonds is converted to kinetic energy and heat body and friction from tires ID: 248317

heat energy temperature efficiency energy heat efficiency temperature transfer law quality radiation thermodynamics 000 car engine maximum work efficient high object total

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Slide1

ThermodynamicsSlide2

1st

law of thermodynamics

Energy may be converted to different forms, but it is neither created nor destroyed during transformations

Energy from chemical bonds is converted to kinetic energy and heat (body and friction from tires)

Amount of energy before and after transformation is the same, only the

form

of the energy has changed

ENERGY

HeatSlide3

1st Law (Contd.)

Another way to state the 1

st

law is mathematically.

D

E = Q + W

This equation says that the only way to change the energy of a

system is to add heat to it (Q) or to do work on it (W)

Example: Can make

wood hotter by applying fire or hittingSlide4

Heat

Heat - the

ENERGY transferred

between objects of different temperature

While used a lot in our vocabulary, this term is

very misunderstood

Heat is NOT temperature. An object CANNOT

contain heat; objects contain thermal energy.

Heat is a very important type of energy transferSlide5

Heat Versus Temperature

Temperature - the property that two objects have in common when

NO heat is transferred between them

Temperature is a relative property. We define it in relationship

to other things

T

1

> T

2

T1 = T

2Slide6

Heat Flow

Conduction - energy transfer by next-nearest molecule

interaction

Convection - energy transfer by mixing; can be naturalor forced (fan, stirring, etc.)Radiation - energy transfer by electromagnetic radiation

Heat can flow via one of three methodsSlide7

Conduction

Energy transfer by nearest molecules running into each other

Rate of heat transfer depends on

Temperature difference

D

T = T

H - TC

Thickness of material LThermal conductivity of material kSurface area A

Q k DT A

t L=Slide8

Conduction

Q

D

T A

t R

=

More familiar

If intervening material is made up of

more than one substance, add R-values

R

total = R1 + R2

+ R3 + ….

Problem: How is the rate of heat transfer affected by adding an

R-value 8 insulation to an 8’x20’ wall that has an R-value of 12when the temperature difference is 20 oF?Slide9

Convection

Heat transfer via mixing; requires some type of fluid (gas, liquid)

Things can naturally convect, especially when density changes

and more buoyant materials will riseForced convection requires energy inputSlide10

Radiation

Every object in the universe emits

electromagnetic radiation because it

has a temperature above absolute zero.

Type of radiation depends upon the

value of the temperature

Wein’s Law =>

lmax =

.003 m K

T

Problem: At what wavelength do you emit most of your radiation?Slide11

Stefan-Boltzmann Law

The rate of heat emission due to radiation depends on size and

temperature.

Q/t = e

s A T

4 where e is the emissivity of the object

Remember, the object will be absorbing radiation while it is

emitting. Therefore, the total heat transfer is

Q/t = e s A (Tobject4 - Tsurroundings4)Slide12

Heat Transfer Devices

Heat Pump

Heat Engine

Transfers heat from cold to hot using external energy W

Example: Refrigerator

Outputs useful energy W by

extracting it from heat passing

from hot to cold

Example: Car engine

In both devices,QH

= QC + WSlide13

If energy is never created or destroyed, why can’t we keep reusing the same energy source forever?

ANSWER

:

Although energy isn’t destroyed, in every energy

transfer, some of it will change to a non-usable form

This is a consequence of the 2

nd

law of thermodynamics

“In a closed system, the total entropy either increases or stays the same”

2

nd

law of thermodynamicsSlide14

Second law of thermodynamics

ENERGY

Waste

Heat

When a chemical bond is broken, you get some high quality

ENERGY

capable of doing work, and some low quality “wasted” energy

No energy was lost or created in the transfer, but the

usability

of the energy declined in the transformation.

This low quality energy cannot be effectively harnessed to do any more work, so you cannot use one energy source foreverSlide15

Example: powering your car

Breaking chemical bonds in gas during combustion yields high quality energy which produces kinetic energy to move car

Also produces waste energy as heat

with little ability to do work

Second law of thermodynamicsSlide16

Combustion

of gasoline

Piston

movement

Axle

turns

Wheels

turn

Heat loss during

combustion

E

Friction

with pistons

E

Friction

with axle

E

Friction

of tires

with road

E

E

E

E

E

Energy in

gasoline

Amount of high quality energy declines with each step (width of orange arrows)

No energy is lost, it simply is converted to low-quality heat that cannot be used for further work

Usable ESlide17

Efficiency

A measure of how well energy is converted

Efficiency =

useful energy out

total energy input

Examples

Internal combustion engine car is about 10% efficient

Electric car is about 20% efficient

Incandescent light bulb is about 1% efficientSlide18

Efficiency Example

A power plant consumes 80,000 Joules of coal energy to

produce 30,000 Joules of electricity. What is the efficiency?

Efficiency =

30,000 J

80,000 J

= .375 = 37.5 %

= 10,000 JSlide19

Heat Engine Efficiency

Energy input = Q

H

Usable energy output = W

Efficiency =

W

Q

H

Since

QH = QC + W => W = QH - QC

Efficiency = 1 -

Q

C

QH

Problem: A car takes in 20,000 J of gasoline and outputs 19,000 J of

heat. What is the efficiency of the car?Slide20

Heat Pump COP

For heat pumps, it is not proper to discuss

efficiency since there is no “usable energy

ouput”. Instead, define “coefficient of

performance” to discuss how much energy

it moves per energy paid for.

COPheater =

COPa.c.

= QH

W

Q

C

W

Note: COP

heater is always greater than 1. Why?Slide21

Maximum Efficiency

Unfortunately, the 2nd law of thermodynamics limits the

maximum efficiency that a device can have. No device will

ever be 100% efficient.

For a heat engine, the limit is given by

Maximum efficiency = 1 -

T

C

T

H

where TC is the temperature of the cold reservoir and TH

is the temperature of the hot reservoir in the Kelvin temperaturescaleSlide22

Maximum Efficiency Example

An inventor proposes a heat engine that will produce electricity

by extracting heat from ocean surface water at 20

oC (293 K) and dumping the waste heat to the deep ocean at 5oC (278 K). What is the maximum efficiency?

Maximum efficiency = 1 -

278 K

293 K

= 1 - .95 = .05

At most, this device will be 5% efficient. In reality, it will

probably only be about half of this, or 2-3% efficient.Slide23

Recapping

2nd LAW

:

Energy is transformed from high quality to low quality

1st LAW

:

Energy is neither created nor destroyed, only transformed

RESULT

:

Low quality heat cannot do substantial work, requiring a new source of high quality energy