The Van der Waals equation is a modified version of the ideal gas law that accounts for the real behavior of gases. It is written as, \[\begin{equation} (P + a(\frac{n^2}{V^2}))(V - nb) = nRT \end{equation}\]where:
- \( P \) is the pressure of the gas,
- \( V \) is the volume of the gas,
- \( n \) is the number of moles,
- \( T \) symbolizes the temperature,
- \( R \) is the ideal gas constant,
- \( a \) and \( b \) are the Van der Waals constants.
The coefficient \( a \) reflects the magnitude of the attractive forces between particles, while \( b \) takes into account the volume occupied by the gas particles themselves. This equation shows us that real gases do not always behave as predicted by the ideal gas law, especially under high pressure and low temperature conditions where the particles are closer together and their actual volume and attractions cannot be ignored.
To understand \( b \) more deeply, it represents the excluded volume – that is the volume a mole of gas molecules actually occupies and is unavailable for other molecules to occupy. Gases with larger molecules have higher values of \( b \), indicating that they need more 'personal space' and thus do not compress as much as gases with smaller molecules under the same pressure.