To determine the relationship between the average force that a molecule applies on the walls of a closed container and the temperature \( T \), let's analyze the behavior of an ideal gas.
According to the kinetic theory of gases, the pressure \( P \) exerted by an ideal gas is given by:
\(P = \frac{1}{3} N m \overline{v^2} / V\)
where:
The mean square velocity \( \overline{v^2} \) is related to the temperature by:
\(\overline{v^2} = \frac{3kT}{m}\)
where:
Substituting \( \overline{v^2} \) in the equation for pressure:
\(P = \frac{1}{3} N \frac{3kT}{V} = \frac{NkT}{V}\)
The average force (\( F \)) exerted by a molecule on the walls is related to the pressure by:
\(F = PA\)
Here, \( A \) is the area of the wall. Since we consider molecular impacts, we can relate force per collision and frequency of collisions, showing how force is proportional to pressure.
From kinetic theory: \(P \propto T\).
Thus, the force is \(F \propto T \), and hence\)
Therefore, the correct estimate for \( q \) is 1, meaning that the average force exerted by a gas molecule depends linearly on the temperature \( T \).