The mean free path \( \lambda \) of molecules is given by the formula:
\[
\lambda = \frac{RT}{\sqrt{2} \pi d^2 N_A P},
\]
where \( R \) is the gas constant, \( T \) is the temperature, \( d \) is the diameter of gas molecules, \( N_A \) is Avogadro's number, and \( P \) is the pressure.
At constant pressure, the mean free path is directly proportional to temperature \( T \):
\[
\lambda \propto T.
\]
Given:
\[
\lambda_\text{STP} = 1500d \quad \text{at} \quad T = 273 \, \text{K}.
\]
For \( T = 373 \, \text{K} \), the new mean free path \( \lambda \) is:
\[
\frac{\lambda}{\lambda_\text{STP}} = \frac{T}{T_\text{STP}}.
\]
Substituting the values:
\[
\frac{\lambda}{1500d} = \frac{373}{273}.
\]
Simplify:
\[
\lambda = 1500d \cdot \frac{373}{273} \approx 2049d.
\]
Thus, the mean free path of the molecules at \( 373 \, \text{K} \) is approximately \( \boxed{2049d} \).