Heat Temperature Heat Transfer Thermal Expansion Thermodynamics Heat

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Heat, Temperature, Heat Transfer, Thermal Expansion & Thermodynamics

Heat, Temperature, Heat Transfer, Thermal Expansion & Thermodynamics

Heat vs. Temperature n Heat n Temperature A form of energy n Measured in

Heat vs. Temperature n Heat n Temperature A form of energy n Measured in calories or Joules n There is no “coldness” energy n Any object with temperature above zero Kelvin has heat energy n n Avg. Kinetic Energy of the particles n Measured in C, F, K, R n “hot” & “cold are relative terms n Absolute zero is zero Kelvin

Heat Transfer (3 methods) 1. Conduction - requires direct contact or particle to particle

Heat Transfer (3 methods) 1. Conduction - requires direct contact or particle to particle transfer of energy; usually occurs in solids 2. Convection - heat moves in currents; only happens in fluid states of matter 3. Radiation - heat waves travel through empty space, no matter needed; IR

Thermal Equilibrium n. A system is in thermal equilibrium when all of its parts

Thermal Equilibrium n. A system is in thermal equilibrium when all of its parts are at the same temperature. n Heat transfers only from high to low temperatures and only until thermal equilibrium is reached.

Temperature Scales n There are four temperature scales – Celsius (Centigrade), Kelvin, Fahrenheit, &

Temperature Scales n There are four temperature scales – Celsius (Centigrade), Kelvin, Fahrenheit, & Rankine n Celsius, C – metric temp. scale n Kelvin, K – metric absolute zero temp. scale n Fahrenheit, F – customary (english) temp. scale n Rankine, R – english absolute zero temp scale

Comparing Temperature Scales All temperatures listed are for water n Celsius - Freezing =

Comparing Temperature Scales All temperatures listed are for water n Celsius - Freezing = 0°C, Boiling = 100°C n Kelvin - Freezing = 273 K, Boiling = 373 K n Fahrenheit- Freezing = 32°F, Boiling = 212°F Conversions between Scales °F = 1. 8 *°C+32 K = °C + 273

Change of State vaporization Heat of fusion w melting 0 -20 ice Temp °

Change of State vaporization Heat of fusion w melting 0 -20 ice Temp ° C 100 freezing r ate m ts ea condensation Heat of vaporization Increasing Heat Energy (Joules) As heat is added to a substance it will either be absorbed to raise the temperature OR to change the state of matter. It can NEVER do both at the same time. Temperature will NOT change during a phase change!

Specific Heat The amount of heat energy needed to raise the temperature of 1

Specific Heat The amount of heat energy needed to raise the temperature of 1 gram of substance by 1°C. Substances with lower specific heats change temperature faster. Symbol : c units : cal/g°C or J/kg°C For water: c = 1 cal/g°C = 4. 18 J/g°C = 4180 J/kg°C

Latent Heat The amount of heat energy required to change the state of 1

Latent Heat The amount of heat energy required to change the state of 1 gram of substance. Heat of fusion - latent heat for changes between the solid and liquid phases. Lf =80 cal/g for water Heat of vaporization - latent heat for changesbetween the solid and liquid phases. Lv =540 cal/g for water

Heat Calculations Temperature Change Q = mcΔT Phase Change Q = m. L Q

Heat Calculations Temperature Change Q = mcΔT Phase Change Q = m. L Q = heat absorbed or released m = mass of substance changing phase m = mass of substance being heated L = latent heat of substance c = specific heat of substance ΔT = change in temperature Lf = heat of fusion (liquid solid) Lv = heat of vaporization (liquid gas)

n Thermodynamics study of changes in thermal properties of matter n Follows Law of

n Thermodynamics study of changes in thermal properties of matter n Follows Law of Conservation of Energy n 1 st Law – the total increase in thermal energy of a system is the sum of the work done on it and the heat added to it n 2 nd Law – natural processes tend to increase the total entropy (disorder) of the universe.

1 st Law of Thermodynamics The total increase in thermal energy of a system

1 st Law of Thermodynamics The total increase in thermal energy of a system is the sum of the work done on it and the heat added to it. ΔU = W + Q ΔU = change in thermal energy of the system W = work done on the system (W = Fd or W=ΔK) Q = heat added to the system (Q is + if absorbed, Q is – if released) *All measured in Joules*

Heat engines n Convert thermal energy to mechanical energy n Require high temp heat

Heat engines n Convert thermal energy to mechanical energy n Require high temp heat source and low temp heat sink. (Takes advantage of heat transfer process) n Examples: Steam engine, Automobile engine

Refrigerators and Heat Pumps n It is possible to remove heat from a cold

Refrigerators and Heat Pumps n It is possible to remove heat from a cold environment and deposit it into a warmer environment. n This requires an outside source of energy. n Examples: Refrigerators, Air conditioning units n Heat pumps are refrigeration units that work in either direction.

2 nd Law of Thermodynamics All natural processes go in a direction that increases

2 nd Law of Thermodynamics All natural processes go in a direction that increases the total entropy of the universe. Entropy is a measure of the disorder of a system. If heat is added, entropy is increased. If heat is removed, entropy is decreased. Work with no ΔT, entropy is unchanged

Thermal Expansion n Substances expand as they heat and contract as they cool. n

Thermal Expansion n Substances expand as they heat and contract as they cool. n The rate of expansion depends on the substance’s coefficient of expansion (α) n The exception to this rule is water. As water is cooled from 4°C to 0°C, it expands which explains why ice floats (it is less dense than water.

Thermal Expansion (Linear) Calculations Lo ΔL Linear expansion: objects expand along linear dimensions such

Thermal Expansion (Linear) Calculations Lo ΔL Linear expansion: objects expand along linear dimensions such as length, width, height, diameter, etc. ΔL = Loα ΔT ΔL = change in length measurement (same units as original length) Lo = original length (may be in any units); ΔT = change in temperature (°C); α = linear coefficient of expansion (/ °C)

Thermal Expansion (Volume) Calculations Volume expansion: since objects expand in all dimensions, volume also

Thermal Expansion (Volume) Calculations Volume expansion: since objects expand in all dimensions, volume also expands. ΔV = Voβ ΔT ΔV = change in volume (same units as original volume) Vo = original volume (may be in any units); ΔT = change in temperature (°C); β = linear coefficient of expansion (/ °C)