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Final exam
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Final exam
Ch. 14: Temperature and Heat
- Zeroth law of thermodynamics
- If systems A and B are in thermal equilibrium and systems B and C are in thermal equilibrium, systems A and C are in thermal equilibrium.
- Temperature is a unique property that determines thermal equilibrium.
- Three different temperature scales:
- Fahrenheit
- Celsius
- Kelvin
- Three different temperature scales:
- Heat
- Heat flow: transfer of energy from one object to another by virtue of a temperature difference
- Heat conduction
- Determined by thermal conductivity, κ
- (Q/T)=κA(ΔT/L)
- Q=heat energy transferred in time t
- L=length of the system
- A=cross-sectional area of the system
- (Q/T)=κA(ΔT/L)
- Determined by thermal conductivity, κ
- Convective heat flow
- Involves the movement of mass and is caused by thermal expansion and contraction
- Radiative heat flow
- Involves electromagnetic radiation
- The total amount of energy an object radiates depends on its temperature.
- Stefan-Boltzmann law
- An object with surface area A and temperature T radiates energy at a rate Q/t
- (Q/t)=σeAT^4
- An object with surface area A and temperature T radiates energy at a rate Q/t
- Wien's law
- The wavelength at which radiation is strongest depends on temperature.
- λmax=(2.90•10^-3 m•K)/T
- Explains why the color of a glowing object depends on its temperature
- The wavelength at which radiation is strongest depends on temperature.
- Stefan-Boltzmann law
- The total amount of energy an object radiates depends on its temperature.
- Involves electromagnetic radiation
- Heat conduction
- Heat flow: transfer of energy from one object to another by virtue of a temperature difference
- Specific heat and latent heat
- If an amount of heat energy Q is added to a substance with mass m, the temperature increases by an amount ΔT
- Q=cmΔT
- c=specific heat
- This equation applies if there is no phase change.
- If there is a phase change such as melting or evaporation, a certain amount of energy called the latent heat must be added to or taken from the system.
- Q=cmΔT
- If an amount of heat energy Q is added to a substance with mass m, the temperature increases by an amount ΔT
- Thermal expansion
- When the temperature of a substance changes, its physical dimensions usually change.
- Changes in length are proportional to the coefficient of thermal expansion α
- (ΔL/Lo)=αΔT
- Changes in volume are proportional to the coefficient of volume expansion β
- (ΔV/Vo)=βΔT
- Changes in length are proportional to the coefficient of thermal expansion α
- When the temperature of a substance changes, its physical dimensions usually change.
- Zeroth law of thermodynamics
Ch. 15: Gases and Kinetic Theory
- Kinetic theory
- Kinetic theory is the application of Newton's laws to the mechanics of a gas of particles
- Leads to the ideal gas law
- For a dilute gas composed of any substance, PV=nRT
- P=pressure, V=volume, n=number of moles of particles, T=temperature, R=universal gas constant=8.31 J/(mol•K)
- Can also be written PV=N(kB)T
- N=number of particles
- kB=Boltzmann's constant=1.38•10^-23 J/K
- For a dilute gas composed of any substance, PV=nRT
- Leads to the ideal gas law
- Kinetic theory is the application of Newton's laws to the mechanics of a gas of particles
- Internal energy
- The temperature of a dilute gas is related to the average kinetic energy of a molecule
- KE=(3/2)(kB)T
- The internal energy of a monatomic ideal gas is equal to the total kinetic energy of the molecules
- U=(3/2)N(kB)T
- For an ideal gas, U is independent of the molecular mass and pressure.
- U=(3/2)N(kB)T
- The temperature of a dilute gas is related to the average kinetic energy of a molecule
- Gas laws
- The ideal gas law contains several other gas laws as special cases.
- Boyle's law
- For a sample of gas at a constant temperature, the product of the pressure and the volume is constant.
- PV=constant
- For a sample of gas at a constant temperature, the product of the pressure and the volume is constant.
- Charles's law
- For a sample of gas at constant pressure, if the temperature is changed by a small amount ΔT, the volume changes by an amount ΔV
- ΔV α ΔT
- For a sample of gas at constant pressure, if the temperature is changed by a small amount ΔT, the volume changes by an amount ΔV
- Gay-Lussac's law
- For a sample of a gas held in a container with a constant volume, changes in pressure are proportional to changes in temperature.
- ΔP α ΔT
- For a sample of a gas held in a container with a constant volume, changes in pressure are proportional to changes in temperature.
- Avogadro's law
- For a sample of gas at a constant pressure and temperature, the volume is proportional to the number of molecules in the sample.
- Boyle's law
- The ideal gas law contains several other gas laws as special cases.
- Specific heat of a gas
- Specific heat per mole of a monatomic ideal gas at constant volume: Cv=(3/2)R
- Diffusion
- The random motion of individual gas molecules
- Δr=√(Dt)
- Δr=average net distance that a molecule diffuses in time t
- D=diffusion constant
- Δr=√(Dt)
- The random motion of individual gas molecules
- Kinetic theory
Ch. 16: Thermodynamics
- Concerned with the behavior of systems containing many particles such as a liquid, gas, or solid.
- Zeroth law of thermodynamics
- If two systems A and B are both in thermal equilibrium with a third system, then A and B are in thermal equilibrium with each other.
- First law of thermodynamics
- If an amount of heat Q flows into a system from its environment and an amount of work W is done by the system on its environment, the internal energy of the system changes by an amount ΔU=Uf-Ui=Q-W
- Second law of thermodynamics
- Can be stated in several different ways.
- Formulation involving heat flow
- Heat flows spontaneously from a warm object to a colder one. It is not possible for heat to flow spontaneously from a cold object to a warmer one.
- Formulation involving heat engines
- The efficiency of a reversible heat engine operating between reservoirs at temperatures T(H) and T(C)
- e=1-T(C)/T(H)
- No heat engine can have a greater efficiency.
- e=1-T(C)/T(H)
- The efficiency of a reversible heat engine operating between reservoirs at temperatures T(H) and T(C)
- Entropy
- In any thermodynamic process, ΔS(universe)≥0
- Formulation involving heat flow
- Can be stated in several different ways.
- Third law of thermodynamics
- It is impossible for the temperature of a system to reach absolute zero.
- Thermodynamic processes
- Isothermal: Temperature remains constant
- Adiabatic process: No heat flow into or out of the system. Q=0
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- Mapa Mental sobre Final exam, criado por bludwig em 03-05-2014.
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