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Heat and Temperature
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Ch4 heat and temperature

Jan 14, 2015

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Page 1: Ch4 heat and temperature

•Heat and Temperature

Page 2: Ch4 heat and temperature

Heat and modern technology are inseparable. These glowing steel slabs, at over 1,100OC (about 2,000OF), are cut by an automatic flame torch. The slab caster converts 300 tons of molten steel into slabs in about 45 minutes. The slabs are converted to sheet steel for

use in the automotive, appliance and building industries.

Page 3: Ch4 heat and temperature

• The Kinetic Molecular Theory.

Page 4: Ch4 heat and temperature

• Introduction.

– Ancient Greeks knew that matter was made up of very small particles.

– Democritus wrote that matter was made up of tiny indivisible particles he called atoms.

• We now know that atoms are not indivisible, but are themselves made up of even smaller particles.

• We have identified more that 200 smaller particles that make up atoms.

Page 5: Ch4 heat and temperature

• Molecules.

– Basic assumption is that matter is made up of tiny units of structure called atoms.

– Atoms are neither created or destroyed during any type of chemical or physical change.

– Arrangements of atoms determines type of entity of matter.

• Elements are pure substances made up of only one type of atom.

• Compounds are made up of one type of atom, but have more complex structures.

Page 6: Ch4 heat and temperature

• Pure substances are composed of 2 or more elements in defined proportions.

• A molecule is the smallest particle of a compound in which all of the atoms maintain their identity.

–maintains all of the chemical and physical properties of the compound.

–Some atoms naturally form molecules called diatomic molecules: O2, F2, Cl2, N2, Br2,

Page 7: Ch4 heat and temperature

Metal atoms appear in the micrograph of a crystal of titanium niobium oxide, magnified 7,800,000 times by

an electron microscope.

Page 8: Ch4 heat and temperature

• Molecules Interact.

– Cohesion.

• Some solids and liquids attract each other and cling to each other.

• Cohesion is when this attractive force is between like molecules.

– Adhesion.

• Some molecules are attracted to other molecules.

Page 9: Ch4 heat and temperature

• Phases of Matter.

– Solids.

• Defined shapes.

• Defines volumes.

• Molecules are fixed distances apart and have strong cohesive forces.

Page 10: Ch4 heat and temperature

– Liquids.• Close together.

• Cohesive forces not as strong as in a solid.

• Defined volume, but not a defined shape.

– Gases

• Weak cohesive forces.

• High kinetic energy.

• Molecules far apart and move in random motion

• No fixed shape or volume.

• Vapor is a gas that is above a liquid phase.

Page 11: Ch4 heat and temperature

(A) In a solid, molecules vibrate around a fixed equilibrium position and are held in place by strong

molecular forces. (B) In a liquid, molecules can rotate and roll over each other because the molecular forces

are not as strong. (C) In a gas, the molecules move rapidly in random free paths.

Page 12: Ch4 heat and temperature

• Molecules Move.

– All molecules have kinetic energy due to movements.

– This kinetic energy can be in the form of:

• Vibrational energy.

• Rotational energy.

• Translational energy where the entire molecule has motion.

Page 13: Ch4 heat and temperature

The basic forms of kinetic energy of molecules. (A) Translational motion is the motion of a molecule as a

whole moving from place to place. (B) Rotational motion is the motion of a turning molecule. (C)

Vibrational motion is the back-and-forth movement of a vibrating molecule.

Page 14: Ch4 heat and temperature

– The kinetic energy of a substance is measured as the temperature of that substance.• Temperature is actually a measure of the

average kinetic energy and has nothing to do with heat until there is a transfer of energy.

Page 15: Ch4 heat and temperature

The number of oxygen molecules with certain velocities that you might find a sample of air at room at temperature. Notice that a few are barely moving and some have velocities over 1,000 m/s at a given time, but the average velocity is somewhere around

500 m/s.

Page 16: Ch4 heat and temperature

• Temperature.

Page 17: Ch4 heat and temperature

• Thermometers.

– Conceptually a thermometer is used to measure the hotness or coldness of an object.

– What a thermometer really measures is the average kinetic energy of an object.

– There is a physical transfer of kinetic energy to the thermometer which them responds due to the increase in its kinetic energy.

• Mercury.

• Ethylene glycol.

Page 18: Ch4 heat and temperature

(A) A bimetallic strip is two different metals, such as iron and brass, bonded together as a single unit,

shown here at room temperatures. (B) Since one metal expands more than the other, the strip

will bend when it is heated. In this example, the brass expands more

than the iron, so the bimetallic strip bends away from the brass.

Page 19: Ch4 heat and temperature

This thermostat has a coiled bimetallic strip that expands and contracts with changes in the room

temperature. The attached vial of mercury is tilted one way or the other, and the mercury completes or breaks

an electric circuit that turns the heating or cooling system on or off.

Page 20: Ch4 heat and temperature

• Thermometer Scales.

– Fahrenheit scale

• Sets boiling point of water at 212 OF and freezing point of water at 32 OF.

• 180 divisions between these two.

• Like most English measures is quite cumbersome.

Page 21: Ch4 heat and temperature

– Celsius scale.• Sets boiling point of water at 100 OC and freezing

point of water at 0 OC.• 100 divisions between these two points.

– Kelvin or absolute scale.• Begins at absolute zero, the temperature at which

all kinetic energy is changed into potential energy.–ie, all molecular motion ceases.

• Boiling point of water is 373 K and freezing point of water is 273 K.

• Divisions are same as for Celsius scale

Page 22: Ch4 heat and temperature

The Fahrenheit, Celsius, and Kelvin temperature scales

Page 23: Ch4 heat and temperature

• Conversions.

– TF = 1.8 TC + 32 OC

– TC = (TF - 32 OF)

• 1.8

• 1.8 accounts for the divisions between freezing point of water and boiling point of water.

–There are 1.8 divisions in the F scale for every 1 division in the C scale.

– TK = TC + 273.

Page 24: Ch4 heat and temperature

– Example.

• The temperature of Lake Superior in August averages 34 OF. What is the temperature in OC.

• Use: TC = (TF - 32 OF)

• 1.8

• TC = (34 OF - 32 OF)

• 1.8

• TC = (2 OF)

• 1.8

Page 25: Ch4 heat and temperature

– Example:• What is the equivalent Celsius temperature of

400.0 K? The equivalent Fahrenheit temperature?

• Use: TK = TC + 273

• Rearrange to : TC = TK - 273

• TC = 400.0 K - 273 = 127.0 OC

• TF = 1.8 (127.0 OC) + 32 OC =

Page 26: Ch4 heat and temperature

• Heat.

Page 27: Ch4 heat and temperature

• Internal and External Energy.

– External energy is total potential and kinetic energy of everyday sized objects.

– Internal energy is the total kinetic and potential energy of an object molecules.

Page 28: Ch4 heat and temperature

One theory about how friction results in increased temperatures: Molecules on one moving surface will

catch on another surface, stretching the molecular forces that are holding it. They are pulled back to their

home position with a snap, resulting in a gain of vibrational kinetic energy.

Page 29: Ch4 heat and temperature

External energy is the kinetic and potential energy that you can see. Internal energy is the total kinetic and

potential energy of molecules. When you push a table across a floor, you do work against friction. Some of

the external mechanical energy goes into internal kinetic and potential energy, and the bottom surface of

the legs becomes warmer.

Page 30: Ch4 heat and temperature

• Heat as Energy Transfer.

– Temperature is a measure of the average kinetic energy of an object.

– Heat is a measure of the internal energy that has been absorbed or transferred from one body to another.

• Increasing the internal energy is called heating.

• Decreasing the internal energy is called cooling.

Page 31: Ch4 heat and temperature

– Two ways to increase temperature:• From a temperature difference, with energy

moving from a region of higher temperature to a region of lower temperature.

• From an object gaining energy by way of a temperature conversion.

Page 32: Ch4 heat and temperature

Heat and temperature are different concepts, as shown by a liter of water (1,000 mL) and a 250 mL cup of water, both at the same temperature. You know the

liter of water contains more heat since it will require more ice cube to cool it, say, 25OC than will be

required for the cup of water. In fact, you will have to remove 48,750 additional calories to cool the liter of

water

Page 33: Ch4 heat and temperature

• Measures of Heat.

– The metric unit of measuring work, energy, or heat is the joule.

– The metric unit of heat is the calorie.

• A calorie is the amount of energy needed to increase the temperature of 1 gram of water 1 OC (from 14.5 OC to 15.5 OC.

• A kilocalorie is the amount of energy needed to increase the temperature of 1 kg of water 1 OC.

Page 34: Ch4 heat and temperature

The Calorie value of food is determined by

measuring the heat released from burning the food. If there is 10.0 kg

of water and the temperature increased from 10OC to 20OC the

food contained 100 Calories (100,000 calories). The food

illustrated here would release much more energy than this.

Page 35: Ch4 heat and temperature

Joule worked with the English system of measurement used during his time. When a 100 lb object falls 7.78

ft, it can do 778 fl?lb of work. If the work is done against friction, as by stirring 1 lb of water, the heat

produced by the wok raises the temperature 1OF.

Page 36: Ch4 heat and temperature

– The English unit of heating is the BTU.• A BTU is the amount of energy needed to

increase the temperature of 1 lb of water 1 OF.

• A Quad is 1 quadrillion BTU 1 X 1015 BTU.

• 778 ftlb = 1 BTU

• 4.184 ftlb = 1 calorie

• 4,184 J = 1 kcalorie

Page 37: Ch4 heat and temperature

– Example: a 2,200.0 kg automobile is moving at 90.0 km/hr (25.0 m/s). How many kilocalories are generated when the car brakes to a stop?

• KE = 1/2mv2

• KE = 1/2(2,200 kg)(25.0m/s)2

• KE = (1,100 kg)(625.0 m2/s2)

• KE = 687,500 m2/s2

• KE = 687,500 J

• Kcal = 687,500 J X 1 kcal/4,184J = 164 kcalories

Page 38: Ch4 heat and temperature

• Specific Heat.– Three variables that influence energy transfer.

• The temperature change.• The mass of the substance.• The nature of the material being heated.

– The amount of heat (Q) needed to increase the temperature (Ti) of a pot of water from the initial temperature to a final temperature (Tf) is proportional to (Tf-Ti).• Q (Tf-Ti).• Q T.

Page 39: Ch4 heat and temperature

– The quantity of heat (Q) absorbed or given off during a certain change in temperature is also proportional to the mass (m) of the substance.

• Q m

– Putting this all together we get:

• Q mcT

• c is the specific heat of the substance.

• Specific heat is the energy needed to increase the temperature of 1 gram of a substance 1 OC.

Page 40: Ch4 heat and temperature

– When two materials of different temperatures are involved in heat transfer and are perfectly insulated from the surroundings, the heat lost by one is equal to the heat gained by the other.• heat lost = heat gained.

• Qlost = Qgained

• (mcT)lost = (mcT)gained

Page 41: Ch4 heat and temperature

Of these three metals, aluminum

needs the most heat per gram per

degree when warmed, and

releases the most heat when cooled.

Page 42: Ch4 heat and temperature

– Example: How much heat must be supplied to a 500.0 g pan to increase its temperature from 20.0 OC to 100.0 OC if the pan is made of a) iron and b) aluminum.• Iron from table 5.2 has a specific heat of 0.11

cal/gOC.• Q = mcT• Q = (500.0g)(0.11 cal/gOC)(80.0OC)• Q = 4,400 cal or 4.40 kcalories• Aluminum from table 5.2 has a specific heat of 0.22

cal/gOC• Q = mcT• Q = (500.0g)(0.22 cal/gOC)(80.0OC)• 8,800 calories or 8.80 kcalories

Page 43: Ch4 heat and temperature

• Heat Flow.

– Conduction.

• Anytime there is a temperature difference; there is a natural tendency for temperature to flow from the area of higher temperature to the area of lower temperature.

• Conduction is the transfer of energy from molecule to molecule.

• The rate depends on the temperature difference, the area and thickness of the substance, and the nature of the material.

Page 44: Ch4 heat and temperature

Thermometers place in holes drilled in a metal rod will show

that heat is conducted from a region of

higher temperature to a region of lower temperature. The

increased molecular activity is passed from molecule to molecule in the

process of conduction.

Page 45: Ch4 heat and temperature

• Some materials are good conductors while others are good insulators.

–Conductors transfer energy very efficiently.

–Insulators transfer energy very inefficiently,

–The best conductors are usually metals which have very little air space between molecules.

–The best insulators have a great deal of air space between molecules.

–The absolute best insulator is a vacuum as there are no molecules to pass on energy.

Page 46: Ch4 heat and temperature

Fiberglass insulation is rated in terms of R-value, a ratio of the conductivity of the material to its

thickness.

Page 47: Ch4 heat and temperature

– Convection.

• Large scale transfer of heat by a large scale displacement of groups of molecules with relatively higher kinetic energy.

• Molecules with higher kinetic energy are moved from one place to another place.

• Happens only in liquids and gases where fluid motion can carry molecules with higher kinetic energy over a distance.

Page 48: Ch4 heat and temperature

(A) Two identical volumes of air are balanced, since they have the same number of molecules and the same mass. (B) Increased temperature causes one volume to

expand from the increased kinetic energy of the gas molecules. (C) The same volume of the expanded air now contains fewer gas molecules and is less dense, and it is buoyed up by the cooler, more dense air.

Page 49: Ch4 heat and temperature

Convection currents move

warm air throughout a

room as the air over the heater

becomes warmed,

expands, and is moved upwards by cooler air.

Page 50: Ch4 heat and temperature

– Radiation.

• Radiation involves the form of energy called radiant energy that moves through space.

• All objects with a temperature above absolute zero give off radiant energy.

• The absolute temperature of the object determines the rate, intensity, and kinds of radiant energy emitted.

Page 51: Ch4 heat and temperature

• Energy, Heat, and Molecular Theory.

Page 52: Ch4 heat and temperature

• Phase Change.

– The motion of a molecule can be increased by:

• Adding heat through a temperature difference.

• The absorption of one of the five forms of energy.

• Temperature increases according to the specific heat of the substance.

Page 53: Ch4 heat and temperature

– When a substance changes from one state to another, the transition is called a phase change.• A phase change always absorbs of releases

energy, a quantity of heat that is not associated with a temperature change.

• Latent heat is the hidden energy of a phase change, which is energy that goes in or comes out of internal potential energy.

Page 54: Ch4 heat and temperature

– Three major types of phase change.

• Solid-liquid.

• Liquid-gas.

• Solid-gas

Page 55: Ch4 heat and temperature

– Solid-liquid.

• The temperature at which a substance changes from a liquid to a solid is called the freezing point.

• The temperature at which a solid changes to a liquid is the melting point.

• Both of these occur at the same temperature.

Page 56: Ch4 heat and temperature

– Liquid-gas.

• The temperature at which a liquid changes from the liquid phase to the gaseous phase is the boiling point.

• The temperature at which a gas or vapor changes to the liquid phase is the condensation point.

• Both of these occur at the same temperature.

Page 57: Ch4 heat and temperature

– Solid-gas.

• A phase change directly from a solid to a gas or vapor is called sublimation.

Page 58: Ch4 heat and temperature

Each phase change absorbs

or releases a quantity of latent heat, which goes into or is

released from molecular potential energy.

Page 59: Ch4 heat and temperature

This graph shows three warming sequences and two phase changes with a constant input of heat. The ice warms to the melting point, then absorbs heat during the phase change as the temperature remains constant. When all the ice has melted, the now liquid water warms to the boiling point, where the temperature again remains constant as heat is absorbed during the second phase change from liquid to gas. After all the liquid has changed to gas, continued warming increases the temperature of the water vapor.

Page 60: Ch4 heat and temperature

(A)Work is done against gravity to lift an object, giving the object more gravitational potential energy.

(B) Work is done against intermolecular forces in separating a molecule from a solid, giving the

molecule more potential energy.

Page 61: Ch4 heat and temperature

Compare this graph to the one in Figure 5.20. This graph shows the relationships between the quantity of heat absorbed during warming and phase changes as water is warmed from ice at -20OC to water vapor at some temperature above 100OC. Note that the specific heat for ice, liquid water, and water vapor (steam) have different values.

Page 62: Ch4 heat and temperature

– Latent heat of fusion.• The latent heat of fusion is the heat involved in a

solid-liquid phase change in melting or freezing.• A melting solid absorbs energy and a freezing

liquid releases this same amount of energy, warming the surroundings.

• The total heat involved in a solid-liquid phase change depends on the mass of the substance involved.

–Q = mLf

–Where Lf is the latent heat of fusion for the substance involved

Page 63: Ch4 heat and temperature

– Latent heat of vaporization.

• The amount of heat involved during a phase change from a liquid to a gas or vapor is called the latent heat of vaporization.

• The latent heat of vaporization is the heat involved in a liquid-gas phase change where there is evaporation or condensation.

• The escaping molecules absorb energy from the surroundings, and a condensing gas releases this exact same amount of energy.

Page 64: Ch4 heat and temperature

• The total heating depends on the amount of water vapor condenses so that:

–Q = mLV

–Where LV is the latent heat of vaporization for the substance involved.

Page 65: Ch4 heat and temperature

• Example:

– How much energy does a refrigerator remove from 100.0 g of water at 20.0 OC to make ice at -10.0 OC

– Three steps.

– Q1 = mcT to cool from 20.0 OC to 0.0 OC

– Q1 = (100.0g)(1.00cal/gOC)(0.0OC-20.0OC)

– = 2,000 cal = 2.00 X 10 3 cal.

Page 66: Ch4 heat and temperature

– Q2 = mLf to remove latent heat of fusion.

– (100.0g)(80.0cal/g)

– 8,000 cal = 8.00 X 103 cal

– Q3 = mcT to go from 0.0 OC to -10 OC

– (100.0g)(0.500cal/g)(10.0OC-0.0OC)

– 500 cal = 5.00 X 102 cal

– Qtotal = Q1 + Q2 + Q3

– = 2.00 X 103 cal + 8.00 X 103 cal + 5.00 X 102 cal

– = 1.05 X 104 cal

Page 67: Ch4 heat and temperature

• Evaporation and Condensation.– Evaporation occurs when enough energy is inputed

into a system to cause liquid molecules to overcome attractive forces near the surface, escape, and become a gas or vapor.

– In evaporation, more molecules are leaving the liquid state than are returning.

– In condensation, more molecules are returning to the liquid state than are leaving.

– When the condensation rate is equal to the evaporation rate, the air above the liquid is saturated (holds all the vapor that it is capable of holding).

Page 68: Ch4 heat and temperature

Temperature is associated with the average energy of the molecules of a substance. These numbered circles represent arbitrary levels of molecular kinetic energy that, in turn, represent temperature. The two molecules with the higher kinetic values [25 in (A)] escape, which lowers the average value from 11.5 to 8.1 (B). Thus evaporation of water molecules with more kinetic energy contributes to the cooling effect of evaporation in addition to the absorption of latent heat.

Page 69: Ch4 heat and temperature

– Four ways to increase the rate of evaporation.

• An increase in temperature of the liquid will increase the average kinetic energy of the molecules and thus increase the number of high energy molecules capable of escaping from the liquid state.

• Increase the surface area of the liquid in contact with the air.

Page 70: Ch4 heat and temperature

• Removal of water vapor from near the surface will prevent the return of molecules to the liquid phase.

• Reducing atmospheric pressure will reduce one of the forces holding molecules in a liquid.

Page 71: Ch4 heat and temperature

• Relative Humidity.

– The ratio of how much water vapor is in air to how much water vapor it could hold at a certain temperature is the relative humidity

– Usually expressed as a percent.

Page 72: Ch4 heat and temperature

The inside of this closed bottle is isolated from the environment so the space above the liquid becomes

saturated. While it is saturated, the evaporation

rate equals the condensation rate. When the bottle is cooled, condensation

exceeds evaporation and droplets of liquid form on

the inside surfaces.

Page 73: Ch4 heat and temperature

The curve shows the maximum amount of water vapor in g/m3 that can be in the air

at various temperatures.

Page 74: Ch4 heat and temperature

• Thermodynamics.

Page 75: Ch4 heat and temperature

• Introduction.

– The laws of thermodynamics describe what happens to energy as it is transformed into work and to other forms.

– Thermodynamics is concerned with internal energy, which is the total internal kinetic and potential energy of a system.

Page 76: Ch4 heat and temperature

– The system is the component we want to describe.

– The state of the system are the variable under which it exists, temperature, pressure, volume, heat, etc…

– Everything outside of the system is the surroundings.

Page 77: Ch4 heat and temperature

A very simple heat engine. The air in (B)

has been heated, increasing the molecular

motion and thus the pressure. Some of the

heat is transferred to the increased gravitational potential energy of the

weight as it is converted to mechanical energy.

Page 78: Ch4 heat and temperature

• The First Law of Thermodynamics.

– The energy supplied to a system is equal to the change in internal energy

Page 79: Ch4 heat and temperature

• The Second Law of Thermodynamics.

– Heat flows from objects with a higher temperature to objects with a cooler temperature.

Page 80: Ch4 heat and temperature

• The Second Law and Natural Processes.

– Energy can be viewed from two considerations of scale:

• The observable external energy of an object.

• The internal energy of the molecules, or particles that make up an object.

Page 81: Ch4 heat and temperature

– Two kinds of motion that the particles of an object can have.• A coherent motion where they move together.

• An incoherent, chaotic motion of individual particles.

– Work on an object is associated with coherent motion, while heating an object is associated with its internal incoherent motion.

Page 82: Ch4 heat and temperature

The heat supplied (QH) to a heat engine goes into

the mechanical work (W) and the remainder is

expelled in the exhaust (QL). The work

accomplished us therefore the difference

in the heat input and output (QH) - (QL), so the

work accomplished represents the heat used,

W = J(QH - QL)

Page 83: Ch4 heat and temperature

A heat pump uses work (W) to move heat from a low temperature region

(QL) to a high temperature region (QH). The heat

moved (QL) requires work (W), so J QL = W.

Page 84: Ch4 heat and temperature

– Entropy.

• Energy is always degrading toward a more disorderly state.

• The total entropy of the universe is continually increasing.

• The natural process is for the sate of order to degrade into a state of disorder with a corresponding increase in entropy.

Page 85: Ch4 heat and temperature

– Eventually all of the useable energy in the universe will diminish to unusable forms.

• The universe will at some time reach a limit of disorder called the heat death of the universe.

• The heat death of the universe is the theoretical limit of disorder, with all molecules spread far, far apart, vibrating slowly with a uniform low temperature.