Step 1: Van der Waals Equation.
The ideal gas equation is:
\[
PV = nRT.
\]
Van der Waals modified it to account for:
1. Finite volume of gas molecules
2. Intermolecular attraction
The van der Waals equation is:
\[
\left(P + \frac{a n^2}{V^2}\right)(V - nb) = nRT.
\]
Where:
$a$ = measure of intermolecular attraction
$b$ = excluded volume of gas molecules
Step 2: Explanation of Corrections.
Pressure correction:
\[
P_{real} = P_{ideal} - \frac{a n^2}{V^2}.
\]
The term $\frac{a n^2}{V^2}$ corrects for intermolecular attraction.
Volume correction:
\[
V_{real} = V_{container} - nb.
\]
The term $nb$ accounts for finite molecular volume.
Step 3: Van der Waals Isotherm (P–V Curve).
When plotting pressure vs volume at constant temperature:
1. At high temperature ($T>T_c$):
Curve resembles ideal gas behaviour (smooth decrease).
2. At critical temperature ($T = T_c$):
Curve shows a point of inflection (critical point).
3. At low temperature ($T<T_c$):
Curve shows a characteristic S-shaped region.
This region represents liquid–gas phase transition.
The flat portion after Maxwell correction represents coexistence of liquid and vapour phases.
Step 4: Critical Constants.
At critical point:
\[
\left(\frac{\partial P}{\partial V}\right)_T = 0
\]
\[
\left(\frac{\partial^2 P}{\partial V^2}\right)_T = 0.
\]
Critical constants are:
\[
V_c = 3nb,
\]
\[
P_c = \frac{a}{27b^2},
\]
\[
T_c = \frac{8a}{27Rb}.
\]
Final Answer:
The van der Waals equation is:
\[
\boxed{
\left(P + \frac{a n^2}{V^2}\right)(V - nb) = nRT
}
\]
and its P–V curve shows deviation from ideal behaviour with a characteristic S-shaped isotherm below critical temperature.