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3. Thermal physics

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3.1 Thermal concepts

Temperature and absolute temperature

There have two commonly used measurment of temperature, one is Celsius(摄氏度) and the other one is Kelvin(开氏度) The temperature difference between them is same ${\Delta K}={\Delta C}$ Absolute zero is 0K whcih is -273$\Celius$

Heat (Internal Energy)

  • Heat is energy that is transferred from one body to another as a result of a difference in temperature.
  • Internal energy is the total random kinetic energy of the particles of a substance, plus the total inter-particle potential energy of the particles.
  • The heat (temperature) is the only determintion of the kenetic energy (温度是衡量动能的唯一标准)

Specific heat capacity

Specific heat capacity follow the formula: $$Q=mc{\Delta T}$$ Q is energy(heat), m is mass, ${\Delta T}$ is Temperature change and c is specific heat capacity.

  • To define this equation, it means that suppose there's a object A have specific heat capacity c and it required Q energy to raise it's temperature 1K(C)
  • Different substances have different specific heat capacities because of different physical properties

Change of phase

When heating some substances it might not necessarily increase temperature but change phase

  • melting (solid to liquid)
  • freezing (liquid to solid)
  • vaporisation/boiling (liquid to gas)
  • condensation (gas to liquid)
  • Sublimation(solid to gas)
  • condensation (gas to solid) phase_change.png

Specific latent heat

Specific latent heat follow the formula: $$Q = mL$$ In this case the L can be replaced by $L_V$ (vaporisation) and $L_F$ (fusion)

  • specific latent heat of fusion: The amount of heat required to change mkg of a substance from solid to liquid without any change in temperature.
  • Specific latent heat of vaporization: The amount of heat required to change mkg of a substance from liquid to gas without any change in temperature.

3.2 Modelling a gas

The Avogadro constant

Avogadro constant $N_A$ is a experimental constant that measurment the number of particle in one mole of substance, which $N_A=6.022\times 10^{23}mol^{-1}$ mole is measured by the amnount of particle carried by 12g of Carbon-12 which repersent as $n$ $$n={\frac{N}{N_A}}$$ Where $n$ is mol number, $N$ is number of particle and $N_A$ is avogadro constnt

Pressure

Pressure is defined as the normal force applied per unit area which followed the equation: $$p={\frac{F}{A}}$$ Where $p$ is pressure $F$ is force and $A$ is area. pressure.png

If the force dose not vertically acting at an object, then should use the equation: $$p=\frac{Fcosθ}{A}$$ p in non-closed condition should be equal to 1atm which is $1.013 × 10^{5}Pa$ on Earth

Ideal gas

An ideal gas is a theoretical model of a gas which should follow the rules that:

  • The molecules are point particles, each with negligible volume.
  • The molecules obey the laws of mechanics.
  • There are no forces between the molecules except when the molecules collide.
  • The duration of a collision is negligible compared to the time between collisions.
  • The collisions of the molecules with each other and with the container walls are elastic.
  • Molecules have a range of speeds and move randomly.

The real gas at high temperature and low pressure will close to ideal gas

An ideal gas should followed the equation: $$PV=nRT$$ P is pressure, V is volume, n is mole number, R is ideal gas constant ($8.31Jmol^{-1}K^{-1}$) and T is temperature

The Boltzmann equation

$$E_{avg}=\frac{3}{2}k_bT$$ This is measurment of average kenetic energy in ideal gas, and $k_b$ means $\frac{R}{N_A}$ which is $1.38\times10^{−23}JK^{−1}$.

Therefore the average internal energy would be: $$U=\frac{3}{2}pV$$