physics final

Cards (83)

  • Work
    The work done on or by a thermodynamic system
  • Thermal Processes for closed systems

    • Isobaric
    • Isovolumetric/Isochoric
    • Isothermal
    • Adiabatic
  • 1st Law of Thermodynamics

    ∆U = Q - W
  • Q
    Energy exchanged between the gas and the environment
  • W
    Work done on/by the gas
  • ∆U
    Internal energy of the gas (sum of kinetic and potential energies of particles)
  • Quasi-static process

    • Occurs slowly enough that a uniform pressure and temperature exists throughout the whole system at all times
  • Isobaric process

    Pressure remains constant
  • Isochoric/Isovolumetric process

    Volume remains constant
  • Isothermal process
    Temperature remains constant
  • Adiabatic process

    No heat is exchanged between the gas and the environment
  • 2nd Law of Thermodynamics
    Defines how spontaneous processes occur
  • Most processes are irreversible - they only happen in one direction
  • 1st definition of 2nd Law of Thermodynamics

    Heat transfer occurs spontaneously from hotter objects to colder objects (never from cold to hot)
  • Heat engine

    • Uses heat to perform work and has 3 essential features: 1) Heat QH is supplied from hot object at TH, 2) Part of input heat is used to do work W, 3) Remaining heat QC is expelled to cold object at TC
  • 2nd definition of 2nd Law of Thermodynamics

    It's impossible for any system to completely convert heat into work during a cyclic process
  • Thermal efficiency of a heat engine

    e = W/QH = 1 - QC/QH
  • Reversible process

    The gas can be returned to its initial state (no spontaneous heat transfers)
  • Carnot engine

    Idealized, maximum-efficiency cyclical engine for reversible processes
  • Carnot efficiency

    eC = 1 - TC/TH
  • 3rd definition of 2nd Law of Thermodynamics
    A Carnot engine will always have a greater efficiency than any other heat engine operating between the same temperatures, and any reversible Carnot engine will always yield the same maximum efficiency for the given operating temperatures
  • Entropy
    A measure of the disorder of a system
  • Entropy change for a reversible process

    ∆S = Q/T
  • 4th definition of 2nd Law of Thermodynamics

    Any reversible process cannot change the entropy of the universe; any irreversible process causes the entropy of the universe to increase (∆S ≥ 0)
  • Specific Heat
    Quantify the amount of heat required to change the temperature of an object
  • Calorimetry
    Learn how insulating materials are used to exchange heat between multiple objects
  • Latent Heat
    Quantify the amount of heat required to change the phase of an object
  • Thermal Processes
    Learn how heat is exchanged between objects through convection, conduction, and radiation
  • Heat (Q)

    The spontaneous transfer of energy between a system and its environment due to a temperature difference
  • Example of heat transfer
    • An ice cube in a cup of warm water – the ice cube is the system, while the cup and warm water is the environment
  • Units of heat

    Joules or calories (1 cal = 4.186 J)
    A Calorie describes the energy content in foods, and is related to the calorie: 1 Cal = 1000 cal = 1 kcal
  • Specific Heat (c)
    The energy Q transferred to a mass m will change its temperature by ΔT
    c ≡ Q/mΔT or Q = mcΔT
  • If ΔT > 0 (the substance gets warmer): Q > 0energy flows into the system
  • If ΔT < 0 (the substance gets colder): Q < 0 → energy flows out of the system
  • Calorimeter
    An insulated container that prohibits heat transfer to the outside environment
    Used to measure the specific heat capacities of unknown substances
  • Calorimetry
    The qualitative measure of heat exchange
  • By conservation of energy: Σ Qgained = Σ Qlost or Σ Q = 0
  • Phases Changes of Matter

    Melt: solid → liquid
    Freeze: liquid → solid
    Evaporation: liquid → gas
    Condensation: gas → liquid or gas → solid
    Sublimation: solid → gas
  • During a phase change, the temperature of the object will not change (as long as it's in thermal equilibrium). Only the internal energy will change.
  • Latent Heat (L)
    The energy Q required to change the phase of a material of mass m
    Q = mL