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Chapter 17 Solids Phase Changes Thermal Processes

Chapter 17 Solids Phase Changes Thermal Processes

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Page 1: Chapter 17 Solids Phase Changes Thermal Processes

Chapter 17Solids

Phase Changes

Thermal Processes

Page 2: Chapter 17 Solids Phase Changes Thermal Processes

Announcements

• No office hours today• Regular office hours Thursday• Office hours from 9:00-3:30 Friday

Page 3: Chapter 17 Solids Phase Changes Thermal Processes

Vapor PressureThe pressure of the gas when it is in equilibrium with the liquid is called the equilibrium vapor pressure, and will depend on the temperature.

A liquid boils at the temperature at which its vapor pressure equals the external pressure.

Page 4: Chapter 17 Solids Phase Changes Thermal Processes

a) Charlottesville

b) Denver (the “mile high” city)

c) the same in both places

d) I’ve never cooked in Denver, so I really don’t know

e) you can boil potatoes?

Boiling PotatoesWill boiled potatoes cook faster in Charlottesville or in Denver?

Page 5: Chapter 17 Solids Phase Changes Thermal Processes

a) Charlottesville

b) Denver (the “mile high” city)

c) the same in both places

d) I’ve never cooked in Denver, so I really don’t know

e) you can boil potatoes?

Boiling PotatoesWill boiled potatoes cook faster in Charlottesville or in Denver?

The lower air pressure in Denver means that the water will boil at a lower temperature... and your potatoes will take longer to cook.

Page 6: Chapter 17 Solids Phase Changes Thermal Processes

Phase Diagram

The vapor pressure curve is only a part of the phase diagram.

When the liquid reaches the critical point, there is no longer a distinction between

liquid and gas; there is only a “fluid” phase.

There are similar curves describing the pressure/temperature of transition from solid to liquid, and solid to gas

Page 7: Chapter 17 Solids Phase Changes Thermal Processes

Fusion Curve

The fusion curve is the boundary between the solid and liquid phases; along that curve they exist in equilibrium with each other.

One of these two fusion curves has a shape that is typical for most materials, but the other has shape specific to water.

Which is which?

(a) Curve 1 is the fusion curve for water

(b) Curve 2 is the fusion curve for water

(c) Trick question: there is no fusion curve for water!

Curve 1

Curve 2

Page 8: Chapter 17 Solids Phase Changes Thermal Processes

Fusion Curve

The fusion curve is the boundary between the solid and liquid phases; along that curve they exist in equilibrium with each other.

One of these two fusion curves has a shape that is typical for most materials, but the other has shape specific to water.

Which is which?

(a) Curve 1 is the fusion curve for water

(b) Curve 2 is the fusion curve for water

(c) Trick question: there is no fusion curve for water!

Curve 1

Curve 2

Page 9: Chapter 17 Solids Phase Changes Thermal Processes

Fusion curve for water

Ice melts under pressure!This is how an ice skate works

Page 10: Chapter 17 Solids Phase Changes Thermal Processes

Phase Equilibrium

The sublimation curve marks the boundary between the solid and gas phases.

The triple point is where all three phases are in equilibrium.

Page 11: Chapter 17 Solids Phase Changes Thermal Processes

Heat and Phase ChangeWhen two phases coexist, the temperature remains the same even if a small amount of heat is added. Instead of raising the temperature, the heat goes into changing the phase of the material – melting ice, for example.

Page 12: Chapter 17 Solids Phase Changes Thermal Processes

Latent HeatThe heat required to convert from one phase to another is called the latent heat.

The latent heat, L, is the heat that must be added to or removed from one kilogram of a substance to convert it from one phase to another. During the conversion process, the temperature of the system remains constant.

Page 13: Chapter 17 Solids Phase Changes Thermal Processes

Latent HeatThe latent heat of fusion is the heat needed to go from solid to liquid;

the latent heat of vaporization from liquid to gas.

Page 14: Chapter 17 Solids Phase Changes Thermal Processes

Boiling Potatoes

Will potatoes cook faster if the water is boiling faster?

a) Yes

b) No

c) Wait, I’m confused. Am I still in Denver?

Page 15: Chapter 17 Solids Phase Changes Thermal Processes

Boiling Potatoes

Will potatoes cook faster if the water is boiling faster?

The water boils at 100°C and remains at that temperature until allof the water has been changed into steam. Only then will the steam increase in temperature. Because the water stays at the same temperature, regardless of how fast it is boiling, thepotatoes will not cook any faster.

Follow-upFollow-up: : How can you cook the potatoes faster?

a) Yes

b) No

c) Wait, I’m confused. Am I still in Denver?

Page 16: Chapter 17 Solids Phase Changes Thermal Processes

You’re in Hot Water!

Which will cause more

severe burns to your skin:

100°C water or 100°C

steam?

a) water

b) steam

c) both the same

d) it depends...

Page 17: Chapter 17 Solids Phase Changes Thermal Processes

Although the water is indeed hot, it releases only 1 cal/(gK1 cal/(gK)) of

heat as it cools. The steam, however, first has to undergo a

phase changephase change into water and that process releases 540 cal/g540 cal/g,

which is a very large amount of heat. That immense release

of heat is what makes steam burns so dangerous.

You’re in Hot Water!

Which will cause more

severe burns to your skin:

100°C water or 100°C

steam?

a) water

b) steam

c) both the same

d) it depends...

Page 18: Chapter 17 Solids Phase Changes Thermal Processes

Phase Changes and Energy Conservation

Solving problems involving phase changes is similar to solving problems involving heat transfer, except that the latent heat must be included as well.

Page 19: Chapter 17 Solids Phase Changes Thermal Processes

Water and Ice You put 1 kg of ice at 0°C

together with 1 kg of water

at 50°C. What is the final

temperature?

– LF = 80 cal/g

– cwater = 1 cal/g °C

a) 0°C

b) between 0°C and 50°C

c) 50°C

d) greater than 50°C

Page 20: Chapter 17 Solids Phase Changes Thermal Processes

How much heat is needed to melt the ice?

QQ = = mLmLff = (1000 = (1000 gg) ) (80 cal/ (80 cal/gg) = 80,000 cal) = 80,000 cal

How much heat can the water deliver by cooling from 50°°C to 0°°C?

QQ = = ccwaterwater mmΔΔTT = (1 cal/ = (1 cal/gg °°C) C) (1000 (1000 gg) ) (50 (50°°C) = 50,000 calC) = 50,000 cal

Thus, there is not enough heat available to melt all the ice!!

Water and Ice You put 1 kg of ice at 0°C

together with 1 kg of water

at 50°C. What is the final

temperature?

– LF = 80 cal/g

– cwater = 1 cal/g °C

a) 0°C

b) between 0°C and 50°C

c) 50°C

d) greater than 50°C

Page 21: Chapter 17 Solids Phase Changes Thermal Processes

a) Add more ice to the icewater

b) add salt to the icewater

c) hold the icewater in an evacuated chamber (vacuum)

d) Jump in the car and drive to a nearby convenience store

Ice Cold Root BeerYou have neglected to chill root beer for your son’s 5th-birthday party. You submerge the cans in a bath of ice and water as you start dinner. How can you hurry the cooling process?

Page 22: Chapter 17 Solids Phase Changes Thermal Processes

a) Add more ice to the icewater

b) add salt to the icewater

c) hold the icewater in an evacuated chamber (vacuum)

d) Jump in the car and drive to a nearby convenience store

Ice Cold Root BeerYou have neglected to chill root beer for your son’s 5th-birthday party. You submerge the cans in a bath of ice and water as you start dinner. How can you hurry the cooling process?

Not a), because ice water at 1 atm is zero degrees, no matter the proportion of water and ice

Not c), because ice is less dense than water so you will raise the melting point when you reduce the pressure. This will allow the water to get a little warmer than 0o

Not d), because you’ll forget your wallet and it will end up taking more time

b) because salt interferes with the formation of ice. This barrier to the solid phase lowers the fusion temperature, and so reduces the temperature of the ice water. (This is why you salt the sidewalk in winter.)

Page 23: Chapter 17 Solids Phase Changes Thermal Processes

Fusion curve for water

Fusion curve for most stuff

remember: water is weird: it melts under pressure, and freezes under vacuum, when near the fusion curve

Again: explaining why putting the ice/water under vacuum won’t help the root beer chill faster

Page 24: Chapter 17 Solids Phase Changes Thermal Processes

As pressure goes lower, the ice/water mixture will ride the fusion curve from point 1 to point 2.This implies that temperature goes up.

Fusion curve for water

1

2ΔP

ΔT

The larger ΔT, the more heat transfers per unit time. Thus, the colder the ice bath, the faster the root beer will chill, and the warmer the bath, the slower the root beer will chill

When two states exist in the same system (like, ice and water), the system MUST be on the equilibrium curve (in the case, the fusion curve).

Page 25: Chapter 17 Solids Phase Changes Thermal Processes

Chapter 18

The Laws of Thermodynamics

Page 26: Chapter 17 Solids Phase Changes Thermal Processes

Reversible (frictionless pistons, etc.) and quasi-static processes

For a process to be reversible, it must be possible to return both the system and its surroundings to the same states they

were in before the process began.

V

P

Quasi-static = slow enough that system is always effectively in equilibrium

area under the curve

W =W

Page 27: Chapter 17 Solids Phase Changes Thermal Processes

a) zero zero

b) -153 J -153 J

c) -41 J

d) -26 J

e) 41 J

Internal EnergyAn ideal gas is taken through the four processes shown. The changes in internal energy for three of these processes is as follows:

The change in internal energy for the process from C to D is:

Page 28: Chapter 17 Solids Phase Changes Thermal Processes

Internal EnergyInternal Energy

a) zero zero

b) -153 J -153 J

c) -41 J

d) -26 J

e) 41 J

An ideal gas is taken through the four processes shown. The changes in internal energy for three of these processes is as follows:

The change in internal energy for the process from C to D is:

PV = nRT

so in a PV cycle, ΔT = 0

ΔT = 0 means that ΔU = 0

ΔUCD = -41 J

Page 29: Chapter 17 Solids Phase Changes Thermal Processes

How much work is done by the gas in this process, in terms of the initial pressure and volume?

One mole of an ideal monatomic gas undergoes the reversible expansion shown in the figure, where V2 = 5 V1 and P2 = 3 P1.

P1

V1 V2 =5V1

P2 = 3P1

a) 4 P1V1

b) 7 P1V1

c) 8 8 P1V1

d) 21 P1V1

e) 29 29 P1V1

Page 30: Chapter 17 Solids Phase Changes Thermal Processes

a) 4 P1V1

b) 7 P1V1

c) 8 8 P1V1

d) 21 P1V1

e) 29 29 P1V1

How much work is done by the gas in this process, in terms of the initial pressure and volume?

One mole of an ideal monatomic gas undergoes the reversible expansion shown in the figure, where V2 = 5 V1 and P2 = 3 P1.

P1

V1 V2 =5V1

P2 = 3P1

Area under the curve:(4 V1)(P1) + 1/2 (4V1)(2P1) = 8 V1P1

Page 31: Chapter 17 Solids Phase Changes Thermal Processes

How much internal energy is gained by the gas in this process, in terms of the initial pressure and volume?

One mole of an ideal monatomic gas undergoes the reversible expansion shown in the figure, where V2 = 5 V1 and P2 = 3 P1.

P1

V1 V2 =5V1

P2 = 3P1

a) 7 P1V1

b) 8 P1V1

c) 15 15 P1V1

d) 21 P1V1

e) 29 P1V1

Page 32: Chapter 17 Solids Phase Changes Thermal Processes

How much internal energy is gained by the gas in this process, in terms of the initial pressure and volume?

One mole of an ideal monatomic gas undergoes the reversible expansion shown in the figure, where V2 = 5 V1 and P2 = 3 P1.

P1

V1 V2 =5V1

P2 = 3P1

a) 7 P1V1

b) 8 P1V1

c) 15 15 P1V1

d) 21 P1V1

e) 29 P1V1

Ideal monatomic gas: U = 3/2 nRT

Ideal gas law: PV = nRT

P2V2 = 15 P1V1

Δ(PV) = 14 P1V1

U = 3/2 PV

ΔU = 21 P1V1

Page 33: Chapter 17 Solids Phase Changes Thermal Processes

How much heat is gained by the gas in this process, in terms of the initial pressure and volume?

One mole of an ideal monatomic gas undergoes the reversible expansion shown in the figure, where V2 = 5 V1 and P2 = 3 P1.

P1

V1 V2 =5V1

P2 = 3P1

a) 7 P1V1

b) 8 P1V1

c) 15 15 P1V1

d) 21 P1V1

e) 29 P1V1

Page 34: Chapter 17 Solids Phase Changes Thermal Processes

How much heat is gained by the gas in this process, in terms of the initial pressure and volume?

One mole of an ideal monatomic gas undergoes the reversible expansion shown in the figure, where V2 = 5 V1 and P2 = 3 P1.

P1

V1 V2 =5V1

P2 = 3P1

a) 7 P1V1

b) 8 P1V1

c) 15 15 P1V1

d) 21 P1V1

e) 29 P1V1

First Law of Thermodynamics

W = 8 P1V1

Page 35: Chapter 17 Solids Phase Changes Thermal Processes

a) at constant pressure at constant pressure

b) if the pressure increases in if the pressure increases in proportion to the volumeproportion to the volume

c) if the pressure decreases in proportion to the volume

d) at constant temperature

e) adiabatically

Internal Energy

An ideal gas undergoes a reversible expansion to 2 times its original volume. In which of these processes does the gas have the largest loss of internal energy?

Page 36: Chapter 17 Solids Phase Changes Thermal Processes

a) at constant pressure at constant pressure

b) if the pressure increases in if the pressure increases in proportion to the volumeproportion to the volume

c) if the pressure decreases in proportion to the volume

d) at constant temperature

e) adiabatically

Internal Energy

An ideal gas undergoes a reversible expansion to 2 times its original volume. In which of these processes does the gas have the largest loss of internal energy?

Since U = 3/2 nRT, and PV=nRT, the largest loss in internal energy corresponds to the largest drop in temperature, and so the largest drop in the product PV.a) PV doubles. Ufinal = 2Uinitial

b) (PV)final = 4 (PV)initial Ufinal = 4Uinitial

c) PV is constant, so U is constantd) U is constante) Adiabatic, so ΔU = -W. This is the only process which reduces U!

Page 37: Chapter 17 Solids Phase Changes Thermal Processes

Specific Heat for an Ideal Gas at Constant Volume

Specific heats for ideal gases must be quoted either at constant pressure or at constant volume. For a constant-volume process,

Page 38: Chapter 17 Solids Phase Changes Thermal Processes

For an ideal gas (from the kinetic theory)

First Law of Thermodynamics

Constant Volume

Page 39: Chapter 17 Solids Phase Changes Thermal Processes

Specific Heat for an Ideal Gas at Constant Pressure

At constant pressure, (some work is done)

Some of the heat energy goes into the mechanical work, so more heat input is required to produce the same ΔT

Page 40: Chapter 17 Solids Phase Changes Thermal Processes

For an ideal gas (from the kinetic theory)

First Law of Thermodynamics

Page 41: Chapter 17 Solids Phase Changes Thermal Processes

Specific Heats for an Ideal Gas

Although this calculation was done for an ideal, monatomic gas, the difference Cp - Cv works well for real gases.

Both CV and CP can be calculated for a monatomic ideal gas using the first law of thermodynamics.

Page 42: Chapter 17 Solids Phase Changes Thermal Processes

Specific Heats and Adiabats In Ideal Gas

The P-V curve for an adiabat is given by

for monotonic gases

Page 43: Chapter 17 Solids Phase Changes Thermal Processes

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• No office hours today• Regular office hours Thursday• Office hours from 9:00-3:30 Friday