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Chapter 17. Quantity Chapter 17. Quantity of Heat of Heat A PowerPoint Presentation by A PowerPoint Presentation by Paul E. Tippens, Professor Paul E. Tippens, Professor of Physics of Physics Southern Polytechnic State Southern Polytechnic State University University © 2007
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Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

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Page 1: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Chapter 17. Quantity of Chapter 17. Quantity of HeatHeat

A PowerPoint Presentation byA PowerPoint Presentation by

Paul E. Tippens, Professor of Paul E. Tippens, Professor of PhysicsPhysics

Southern Polytechnic State Southern Polytechnic State UniversityUniversity© 2007

Page 2: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

FOUNDRY: It requires about 289 Joules of heat to melt one gram of steel. In this chapter, we will define the quantity of heat to raise the temperature and to change the phase of a substance.

Photo © Vol. 05 Photodisk/Getty

Page 3: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Objectives: After finishing Objectives: After finishing this unit, you should be this unit, you should be able to:able to:

• Define the quantity of heat in terms of the calorie, the kilocalorie, the joule, and the Btu.

• Write and apply formulas for specific heat capacity and solve for gains and losses of heat.

• Write and apply formulas for calculating the latent heats of fusion and vaporization of various materials.

Page 4: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Heat Defined as EnergyHeat Defined as Energy

Heat is not something an object has, but rather energy that it absorbs or gives up. The heat lost by the hot coals is equal to that gained by the water.

Heat is not something an object has, but rather energy that it absorbs or gives up. The heat lost by the hot coals is equal to that gained by the water.

Hot coals

Cool water

Thermal Equilibrium

Page 5: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Units of HeatUnits of Heat

One calorie (1 cal) is the quantity of heat required to raise the temperature of 1 g of water by 1 C0.

10 calories of heat will raise the temperature of 10 g of water by 10 C0.

ExamplExamplee

Page 6: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Units of Heat (Cont.)Units of Heat (Cont.)

10 kilocalories of heat will raise the temperature of 10 kg of water by 10 C0.

ExamplExamplee

One kilocalorie (1 kcal) is the quantity of heat required to raise the temperature of 1 kg of water by 1 C0.

Page 7: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Units of Heat (Cont.)Units of Heat (Cont.)

10 Btu of heat will raise the temperature of 10 lb of water by 10 F0.

ExamplExamplee

One British Thermal Unit (1 Btu) is the quantity of heat required to raise the temperature of 1 lb of water by 1 F0.

Page 8: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

The Btu is an Outdated The Btu is an Outdated UnitUnit

The British Thermal Unit (1 Btu) is discouraged, but unfortunately remains in wide-spread use today. If it is to be used, we must recognize that the pound unit is actually a unit of mass, not weight.

1 lb (1/32) slug

When working with the BtuBtu, we must recall that the pound-masspound-mass is not a variable quantity that depends on gravity --

one reason that the use of one reason that the use of the Btu is discouraged!the Btu is discouraged!

1 lb

Page 9: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

The SI Unit of HeatThe SI Unit of Heat

Since heat is energy, the joule is the preferred unit. Then, mechanical energy and heat are

measured in the same fundamental unit.

Since heat is energy, the joule is the preferred unit. Then, mechanical energy and heat are

measured in the same fundamental unit.

1 cal = 4.186 J1 cal = 4.186 J

Comparisons of Heat Units:Comparisons of Heat Units:

1 kcal = 4186 J1 kcal = 4186 J

1 Btu = 778 ft lb1 Btu = 778 ft lb

1 Btu = 252 cal1 Btu = 252 cal

1 Btu = 1055 J1 Btu = 1055 J

Page 10: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Temperature and Quantity of Temperature and Quantity of HeatHeat

200 g

600 g

200C

200C

220C

300C

The effect of heat on temp- erature depends on the quantity of matter heated.

The same quantity of heat is applied to each mass of water in the figure.

The larger mass experiences a smaller increase in temperature.

Page 11: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Heat CapacityHeat CapacityThe heat capacity of a substance is the heat required to raise the temperature a unit degree.

Lead Glass Al Copper Iron

Heat capacities based on time to heat from zero to 1000C. Which has the greatest heat capacity?

37 s 52 s 60 s 83 s 90 s

1000C 1000C 1000C 1000C 1000C

Page 12: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Heat Capacity (Continued)Heat Capacity (Continued)

Lead Glass Al Copper Iron

Iron and copper balls melt all the way through; others have lesser heat capacities.

All at 1000C placed on Paraffin SlabAll at 1000C placed on Paraffin Slab

Lead Glass Al Copper Iron

Page 13: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Specific Heat CapacitySpecific Heat CapacityThe specific heat capacity of a material is the quantity of heat needed to raise the temperature of a unit mass through a unit degree.

The specific heat capacity of a material is the quantity of heat needed to raise the temperature of a unit mass through a unit degree.

; Q

c Q mc tm t

; Q

c Q mc tm t

Water: c = 1.0 cal/g C0 or 1 Btu/lb F0 or 4186 J/kg KWater: c = 1.0 cal/g C0 or 1 Btu/lb F0 or 4186 J/kg K

Copper: c = 0.094 cal/g C0 or 390 J/kg KCopper: c = 0.094 cal/g C0 or 390 J/kg K

Page 14: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Comparison of Heat Units:Comparison of Heat Units: How much How much heat is needed to raise 1-kg of water from heat is needed to raise 1-kg of water from 0000 to 100 to 10000C?C?The mass of one kg of water is:

1 kg = 1000 g = 0.454 lbm

1 kgQ mc t For water: c = 1.0 cal/g C0 or 1 Btu/lb F0 or 4186 J/kg K

1 lbm = 454 g

The heat required to do this The heat required to do this job is:job is:10,000 cal 10 kcal

39.7 Btu 41, 860 J

Page 15: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Problem Solving ProcedureProblem Solving Procedure

; Q

c Q mc tm t

Water: c = 1.0 cal/g C0 or 1 Btu/lb F0 or 4186 J/kg KWater: c = 1.0 cal/g C0 or 1 Btu/lb F0 or 4186 J/kg K

1. Read problem carefully and draw a rough sketch.

2. Make a list of all given quantities

3. Determine what is to be found.

4. Recall applicable law or formula and constants.

5. Determine what was to be found.

Page 16: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Example 1:Example 1: AA 500-g 500-g copper coffee copper coffee mug is filled with mug is filled with 200-g200-g of coffee. of coffee. How much heat was required to How much heat was required to heat cup and coffee from heat cup and coffee from 2020 to to 969600CC??1. Draw sketch of problem1. Draw sketch of problem.

2. List given information.2. List given information.

Mug massMug mass mmmm = = 0.500 kg0.500 kg

Coffee massCoffee mass mmcc = = 0.200 kg0.200 kg

Initial temperature of coffee and mug:Initial temperature of coffee and mug: tt00 = 20 = 2000CCFinal temperature of coffee and mug:Final temperature of coffee and mug: ttff = 96 = 9600CC

Total heat to raise temp-

erature of coffee (water) and mug to 960C.

3. List what is to be found: 3. List what is to be found:

Page 17: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Example 1(Cont.):Example 1(Cont.): How much heat needed How much heat needed to heat cup and coffee from to heat cup and coffee from 2020 to to 969600CC?? mmmm = = 0.2 kg0.2 kg; m; mw w = = 0.5 kg0.5 kg..

4. Recall applicable formula or law:4. Recall applicable formula or law:

Q = mc tHeat Gain or Loss:

5. Decide that TOTAL heat is that 5. Decide that TOTAL heat is that required to raise temperature of mug required to raise temperature of mug and water (coffee). Write equation.and water (coffee). Write equation.

QQTT = = mmmmccmm t + mt + mwwccw w tt

6. Look up specific 6. Look up specific heats in tables:heats in tables:

Copper: cCopper: cmm = 390 J/kg C = 390 J/kg C00 Coffee (water): cCoffee (water): cww = 4186 J/kg C = 4186 J/kg C00

Page 18: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

t = 960C - 200C = 76 C0

t = 960C - 200C = 76 C0

Water: (0.20 kg)(4186 J/kgC0)(76 C0)

Cup: (0.50 kg)(390 J/kgC0)(76 C0)

QT = 63,600 J + 14,800 J

QT = 78.4 kJQT = 78.4 kJ

7. Substitute info and solve problem:7. Substitute info and solve problem:

QT = mmcm t + mwcw t

Copper: cCopper: cmm = 390 J/kg C = 390 J/kg C00 Coffee (water): cCoffee (water): cww = 4186 J/kg C = 4186 J/kg C00

Example 1(Cont.):Example 1(Cont.): How much heat How much heat needed to heat cup and coffee from needed to heat cup and coffee from 2020 to to 969600CC?? mmcc = = 0.2 kg0.2 kg; m; mw w = = 0.5 kg0.5 kg..

Page 19: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

A Word About UnitsA Word About Units

The substituted units must be consistent with those of The substituted units must be consistent with those of the chosen value of specific heat capacity.the chosen value of specific heat capacity.

QQ == mmwwccw w tt

For example: Water cw = 4186 J/kg C0 or 1 cal/g C0

The units for The units for QQ, , m, m, and and t t must be consistent with must be consistent with those based on the value of those based on the value of the constant the constant c.c.

If you use 4186 J/kg C0 for c, then Q must be in joules, and m must be in kilograms.

If you use 4186 J/kg C0 for c, then Q must be in joules, and m must be in kilograms.

If you use 1 cal/g C0 for c, then Q must be in calories, and m must be in grams.

If you use 1 cal/g C0 for c, then Q must be in calories, and m must be in grams.

Page 20: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Conservation of EnergyConservation of EnergyWhenever there is a transfer of heat within a system, the heat lost by the warmer bodies must equal the heat gained by the cooler bodies:

Hot iron

Cool water

Thermal Equilibrium

(Heat Losses) = (Heat Gained) (Heat Losses) = (Heat Gained)

Page 21: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Example 2:Example 2: A handful of A handful of copper shot is heated to copper shot is heated to 909000CC and then dropped into and then dropped into 80 g80 g of of water in an insulated cup at water in an insulated cup at 101000CC. If the equilibrium . If the equilibrium temperature is temperature is 181800CC, what was , what was the mass of the copper?the mass of the copper?

900 shot

100 water

Insulator

te= 180Ccw = 4186 J/kg C0; cs = 390 J/kg C0

mw = 80 g; tw= 100C; ts = 900C

Heat lost by shot = heat gained by watermscs(900C - 180C) = mwcw(180C - 100C)

Note: Temperature differences are [High - Low] to insure absolute values (+) lost and gained.

Page 22: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

2679 J0.0954 kg

28,080 J/kgsm ms = 95.4 gms = 95.4 g

ms(390 J/kgC0)(72 C0) = (0.080 kg)(4186 J/kgC0)(8 C0)

mscs(900C - 180C) = mwcw(180C - 100C)

900 shot

100 water

Insulator

180C

Heat lost by shot = heat gained by water

Example 2: (Cont.)Example 2: (Cont.)

80 g of Water

ms = ?

Page 23: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Change of PhaseChange of Phase

Solid LiquidGas

Q = mLf Q = mLv

fusion

Vaporization

When a change of phase occurs, there is only a change in potential energy of the molecules. The temperature is constant during the change.

When a change of phase occurs, there is only a change in potential energy of the molecules. The temperature is constant during the change.

Terms: Fusion, vaporization, condensation, latent heats, evaporation, freezing point, melting point.

Terms: Fusion, vaporization, condensation, latent heats, evaporation, freezing point, melting point.

Page 24: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Change of PhaseChange of Phase

The The latent heat of fusionlatent heat of fusion ( (LLff) of a substance is ) of a substance is

the heat per unit mass required to change the the heat per unit mass required to change the substance from the solid to the liquid phase of substance from the solid to the liquid phase of its melting temperature.its melting temperature.

The The latent heat of vaporizationlatent heat of vaporization ( (LLvv)) of a of a

substance is the heat per unit mass required substance is the heat per unit mass required to change the substance from a liquid to a to change the substance from a liquid to a vapor at its boiling temperature.vapor at its boiling temperature.

For Water: Lf = 80 cal/g = 333,000 J/kgFor Water: Lf = 80 cal/g = 333,000 J/kg

For Water: Lv = 540 cal/g = 2,256,000 J/kgFor Water: Lv = 540 cal/g = 2,256,000 J/kg

f

QL

mf

QL

m

v

QL

mv

QL

m

Page 25: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Melting a Cube of CopperMelting a Cube of CopperThe heat The heat QQ required to melt a required to melt a substance at its melting temperature substance at its melting temperature can be found if the can be found if the massmass and latent and latent heat of fusionheat of fusion are known. are known.

Q = mLvQ = mLv

2 kgWhat Q to melt copper?

Lf = 134 kJ/kg

Example:Example: To completely melt To completely melt 2 kg of copper at 10402 kg of copper at 104000C, we need:C, we need:Q = mLQ = mLff = (2 kg)(134,000 = (2 kg)(134,000

J/kg)J/kg) Q = 268 kJQ = 268 kJ

Page 26: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Example 3:Example 3: How much heat is needed to How much heat is needed to convert convert 10 g10 g of ice at of ice at -20-2000CC to steam at to steam at 10010000CC??

First, let’s review the process graphically as shown:temperature

t

Qice

steam only

-200C

00C

1000

C

steam and

water

540 cal/g

ice and water

80 cal/gwater only

1 cal/gC0

ice steam

cice= 0.5 cal/gC0

Page 27: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Example 3 (Cont.):Example 3 (Cont.): Step one is Q Step one is Q11 to to convert 10 g of ice at convert 10 g of ice at -20-2000CC to ice at to ice at 0000CC (no water yet).(no water yet).

t

Qice-200C

00C

1000

C

cice= 0.5 cal/gC0

Q1 = (10 g)(0.5 cal/gC0)[0 - (-200C)]

Q1 = (10 g)(0.5 cal/gC0)(20 C0)

Q1 = 100 calQ1 = 100 cal

-200C

00C

Q1 to raise ice to 00C: Q1 = mct

Page 28: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

t

Q-200C

00C

1000

C

Example 3 (Cont.):Example 3 (Cont.): Step two is Q Step two is Q22 to to convert 10 g of ice at convert 10 g of ice at 0000CC to water at to water at 0000CC..

MeltingQ2 to melt 10 g of ice at 00C: Q2 = mLf

80 cal/g

ice and water

Q2 = (10 g)(80 cal/g) = 800 cal

Q2 = 800 calQ2 = 800 cal

Add this to Q1 = 100 cal: 900 cal used to this point.

Page 29: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

t

Q-200C

00C

1000

C

water only

1 cal/gC0

Example 3 (Cont.):Example 3 (Cont.): Step three is Q Step three is Q33 to to change change 10 g10 g of water at of water at 0000CC to water at to water at 10010000CC..

00C to 1000C

Q3 to raise water at 00C to 1000C.Q3 = mct ; cw= 1

cal/gC0 Q3 = (10 g)(1 cal/gC0)(1000C - 00C)

Q3 = 1000 calQ3 = 1000 cal

Total = Q1 + Q2 + Q3

= 100 +900 + 1000 = 1900 cal

Page 30: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Example 3 (Cont.):Example 3 (Cont.): Step four is Q Step four is Q44 to to convert 10 g of water to steam at convert 10 g of water to steam at 10010000CC? ? ((QQ44 = mL = mLvv))

Q-200C

00C

1000

C

vaporization

Q4 to convert all water at 1000C to steam at 1000C. (Q = mLv)

Q4 = (10 g)(540 cal/g) = 5400 cal

100 cal

icewater only

ice and water

800 cal1000 cal steam

and water

5400 cal Total Heat:

7300 cal7300 cal

Page 31: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Example 4:Example 4: How many grams of ice at How many grams of ice at 0000CC must be mixed with four grams of must be mixed with four grams of steam in order to produce water at steam in order to produce water at 606000CC??

Ice must Ice must meltmelt and then and then riserise to 60 to 6000C. C. Steam must Steam must condensecondense and and dropdrop to 60 to 6000C.C.

Total Heat Gained = Total Heat Lost

miLf + micwt = msLv + mscwt

Note: All losses and gains are absolute values (positive).Note: All losses and gains are absolute values (positive).

Total Gained: mi(80 cal/g) + mi(1 cal/gC0)(60 C0 - 00C )

Lost: (4 g)(540 cal/g) + (4 g)(1 cal/gC0)(100 C0 - 600C )

Total Gained: mi(80 cal/g) + mi(1 cal/gC0)(60 C0)

Total Lost: (4 g)(540 cal/g) + (4 g)(1 cal/gC0)(40 C0)

mi = ?

4 g

te = 600C

ice

steam

Page 32: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Total Gained: mi(80 cal/g) + mi(1 cal/gC0)(60 C0)

Total Lost: (4 g)(540 cal/g) + (4 g)(1 cal/gC0)(40 C0)

mi = ?

4 g

te = 600C

80mi + 60mi = 2160 g +160 g

Total Heat Gained = Total Heat Lost

2320 g

140im mi = 16.6 g

mi = 16.6 g

Example 4 (Continued)Example 4 (Continued)

Page 33: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Example 5:Example 5: Fifty gramsFifty grams of of ice are mixed with ice are mixed with 200 g200 g of of water initially at water initially at 707000CC. Find . Find the equilibrium the equilibrium temperature of the temperature of the mixture.mixture.

Ice melts and rises to te Water drops from 70 to te.

Heat Gained: miLf + micwt ; t = te - 00C

Gain = 4000 cal + (50 cal/g)te

Gain = (50 g)(80 cal/g) + (50 g)(1 cal/gC0)(te - 00C )

00C 700C

te = ?

50 g 200 g

ice water

Page 34: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Example 5 (Cont.):Example 5 (Cont.):

00C 700C

te = ?

50 g 200 g

GainGain = 4000 cal + (50 cal/g)te

Lost = (200 g)(1 cal/gC0)(700C- te )

Heat Lost = mwcwt

Lost = 14,000 cal - (200 cal/C0) te

t = 700C - te [high - low]

Heat Gained Must Equal the Heat Lost:4000 cal + (50 cal/g)te = 14,000 cal - (200 cal/C0) te

Page 35: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

00C 700C

te = ?

50 g 200 g

Simplifying, we have:(250 cal/C0) te = 10,000 cal

00

10,000 cal40 C

250 cal/Cet

te = 400Cte = 400C

Heat Gained Must Equal the Heat Lost:4000 cal + (50 cal/g)te = 14,000 cal - (200 cal/C0) te

Example 5 (Cont.):Example 5 (Cont.):

Page 36: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Summary of Heat UnitsSummary of Heat UnitsOne calorie (1 cal) is the quantity of heat required to raise the temperature of 1 g of water by 1 C0.

One kilocalorie (1 kcal) is the quantity of heat required to raise the temperature of 1 kg of water by 1 C0.

One British thermal unit (Btu) is the quantity of heat required to raise the temperature of 1 lb of water by 1 F0.

Page 37: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Summary: Change of Summary: Change of Phase Phase

The The latent heat of fusionlatent heat of fusion ( (LLff) of a substance is ) of a substance is

the heat per unit mass required to change the the heat per unit mass required to change the substance from the solid to the liquid phase of substance from the solid to the liquid phase of its melting temperature.its melting temperature.

For Water: Lf = 80 cal/g = 333,000 J/kgFor Water: Lf = 80 cal/g = 333,000 J/kg

f

QL

mf

QL

m

The The latent heat of vaporizationlatent heat of vaporization ( (LLvv)) of a of a

substance is the heat per unit mass required substance is the heat per unit mass required to change the substance from a liquid to a to change the substance from a liquid to a vapor at its boiling temperature.vapor at its boiling temperature.

For Water: Lv = 540 cal/g = 2,256,000 J/kgFor Water: Lv = 540 cal/g = 2,256,000 J/kg

v

QL

mv

QL

m

Page 38: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Summary: Specific Heat Summary: Specific Heat CapacityCapacity

The specific heat capacity of a material is the quantity of heat to raise the temperature of a

unit mass through a unit degree.

The specific heat capacity of a material is the quantity of heat to raise the temperature of a

unit mass through a unit degree.

; Q

c Q mc tm t

; Q

c Q mc tm t

Page 39: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Summary: Conservation of Summary: Conservation of EnergyEnergy

Whenever there is a transfer of heat within a system, the heat lost by the warmer bodies must equal the heat gained by the cooler bodies:

(Heat Losses) = (Heat Gained) (Heat Losses) = (Heat Gained)

Page 40: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

Summary of Formulas:Summary of Formulas:

; Q

c Q mc tm t

; Q

c Q mc tm t

(Heat Losses) = (Heat Gained) (Heat Losses) = (Heat Gained)

; v v

QL Q mL

m ; v v

QL Q mL

m

; f f

QL Q mL

m ; f f

QL Q mL

m

Page 41: Chapter 17. Quantity of Heat A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University © 2007.

CONCLUSION: Chapter 17CONCLUSION: Chapter 17Quantity of HeatQuantity of Heat