Thermal Physics & Ideal Gases

    Cards (47)

    • Thermal equilibrium
      A state where there is no net flow of thermal energy between objects involved, i.e., the objects are at the same temperature
    • Celsius scale
      Relies on the melting and boiling points of water under atmospheric pressure
    • Thermodynamic scale
      Measured in kelvin, uses the triple point of water (273.16K) and absolute zero
    • T (˚K) = T (˚C) + 273
    • Solids
      Have tightly packed atoms, kept together by strong electrostatic forces of attraction; they have kinetic energy which allows them to vibrate in place
    • Liquids
      Have a greater mean separation than solids but are still close together; they have more kinetic energy than solids which means they can change position and flow past each other
    • Gases
      Have molecules that are far apart, with more kinetic energy than those in liquids; they are free to move past each other and collide elastically, moving in random directions with random speeds
    • Brownian motion
      Where molecules of a gas travel in random directions with random velocities
    • Brownian motion can be seen by looking at smoke particles in the air, which are visible under a microscope and shows random motion because it collides with the air molecules
    • Internal energy
      Sum of the kinetic and potential energies in a substance
    • When a substance is heated
      The kinetic energy increases but the potential energy remains the same
    • When a substance changes state
      Potential energy increases but the kinetic energy remains the same
    • Temperature remains the same when the substance changes state as the thermal energy goes to breaking the electrostatic forces
    • Absolute zero is at 0˚K, the temperature at which the particles have no kinetic energy/minimum internal energy; they stop moving completely
    • Specific heat capacity
      Energy required per unit mass to increase the temperature by 1˚K
    • E = mc∆ø
    • Specific latent heat of fusion
      The energy required for 1kg of substance to change state from solid to liquid
    • Specific latent heat of vaporisation
      The energy required for 1kg of substance to change state from liquid to gas
    • Amount of substance
      Measured in moles
    • One mole has 6.02 x 10^23 particles (Avogadro’s constant)
    • n = m / M where n = number of moles, m = mass, M = number of molecules
    • Kinetic theory of gases

      Used to describe how ideal gases behave
    • Assumptions about ideal gases
      • There are a large number of particles
      • Volume of the gas atoms are negligible compared to the large volume
      • Collisions are perfectly elastic
      • Time taken is negligible
      • Electrostatic forces are negligible
    • Collisions inside a container are perfectly elastic so there is a change in momentum which leads to an increase in force
    • Using Newton's third law, an atom exerts an equal and opposite force on the wall
    • Total pressure
      The total force of each atom of gas with the container’s walls and the area of the wall
    • Boyle’s law
      For a fixed mass at a constant temperature, pressure is inversely proportional to the volume
    • Charles’ law
      For a fixed mass of gas at a constant pressure, the volume is directly proportional to temperature
    • pV = nRT where n = number of moles, R = ideal gas constant
    • Experiment to determine absolute zero
      1. Place a sealed container of air connected to a pressure gauge in a water bath
      2. Vary the temperature and record both the pressure and temperature
      3. Plot a graph of pressure against temperature
      4. Plot a line of best fit
      5. Extrapolate the graph until pressure = 0, and this is equal to absolute 0
    • Root mean squared
      Related to the mean kinetic energy of a gas and the pressure
    • Root mean squared is found by summing all of the squares of the velocities and dividing by the number of molecules and the square root of this value
    • The root mean squared can be used to find pressure
    • pV = 1/3 Nmc^2 where N = number of molecules, m = mass of a single particle, c = root mean squared
    • Maxwell Boltzmann distribution
      Shows the number of molecules with each speed
    • The area under the distribution represents the total number of molecules
    • As the temperature increases
      The peak shifts to a higher speed and the distribution becomes more spread out
    • Boltzmann constant (k)

      k = R / Na
    • Boltzmann constant can be used to derive pV = NkT
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