B3-4. Kinetic Theory and Internal Energy
1. Kinetic Theory of Gases
The kinetic theory connects the macroscopic properties of a gas (like pressure and temperature) to the microscopic motion of its constituent particles.
Assumptions of an Ideal Gas:
An ideal gas is a theoretical construct. For a real gas to act "ideally" (which happens best at high temperatures and low pressures), we assume:
- Particles have negligible volume compared to the total volume of the container.
- Collisions between particles and the container walls are perfectly elastic (no kinetic energy is lost).
- There are absolutely no intermolecular forces between particles (except during collisions).
- The duration of collisions is negligible compared to the time between collisions.
2. Average Kinetic & Internal Energy
Because we assume there are absolutely no intermolecular forces in an ideal gas, the particles have exactly zero potential energy. Therefore, the total Internal Energy ($U$) of an ideal gas is purely the sum of the kinetic energies of all its particles.
Average Kinetic Energy of a Single Molecule ($E_K$):
Total Internal Energy of the Gas ($U$):
To find the total internal energy, we simply multiply the average kinetic energy of a single molecule by the total number of molecules ($N$), or apply it in moles ($n$).
- $U$: Total Internal Energy (J)
- $E_K$: Average kinetic energy of one molecule (J)
- $T$: Absolute temperature (K)
Example 1: Internal Energy of Helium
Problem: Calculate the temperature of $3.0$ g of helium gas kept at a constant volume in a cylinder, if its total internal energy is $600$ J. (Helium has a mass number of $4$).
Solution:
- Step 1: Calculate the number of moles ($n$).
The molar mass ($M$) of Helium is $4$ g mol⁻¹.
$n = \dfrac{m}{M} = \dfrac{3.0}{4.0} = 0.75$ mol - Step 2: State the relevant Internal Energy equation.
$$U = \dfrac{3}{2} n R T$$ - Step 3: Rearrange for Temperature ($T$) and solve.
$$T = \dfrac{2U}{3nR} = \dfrac{2 \times 600}{3 \times 0.75 \times 8.31} = \dfrac{1200}{18.6975} \approx \mathbf{64 \text{ K}}$$