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Question: The average kinetic energy of the particles of a gas is most closely associated with which of the fo...

The average kinetic energy of the particles of a gas is most closely associated with which of the following quantity?
A) Heat capacity
B) temperature
C) specific heat
D) absolute zero
E) potential energy

Explanation

Solution

The particles of a gas are supposed to have elastic collisions both with the wall of the container and the other particles ideally. They are thought of as point mass particles with a velocity range zero to infinity. Hence, their average kinetic energy is to be calculated taking care of this assumptions.

Complete step by step answer:
Step 1:

Let in an one dimensional case, a gas particle with mass mm collides with the wall of a container with length dd perpendicularly with a velocity vv and exerts a force FF as

F=mv(mv)t F=2mvt  F = \dfrac{{mv - \left( { - mv} \right)}}{t} \\\ \Rightarrow F = \dfrac{{2mv}}{t} \\\

You can find the frequency of the collision as
1t=vd\dfrac{1}{t} = \dfrac{v}{d}
So, the average force becomes
F=mv2dF = \dfrac{{m{v^2}}}{d}
Step 2:
Calculate the total force on the wall due to all the particles
F=mv2d =mNL[v2N] =mNLvrms2  F = \sum {\dfrac{{m{v^2}}}{d}} \\\ = \dfrac{{mN}}{L}\left[ {\dfrac{{\sum {{v^2}} }}{N}} \right] \\\ = \dfrac{{mN}}{L}v_{rms}^2 \\\
Step 3:
You can exploit the symmetry, hence for a three-dimensional case
vxyz2=vx2+vy2+vz2=3v2v_{xyz}^2 = v_x^2 + v_y^2 + v_z^2 = 3{v^2}
Hence, you get the force FF as
F=mN3dvrms2F = \dfrac{{mN}}{{3d}}v_{rms}^2
Calculate the pressure on the wall of the container as
P=mN3d3vrms2P = \dfrac{{mN}}{{3{d^3}}}v_{rms}^2
Now the volume of the container is the total volume of the gas particles as
V=d3V = {d^3}
Hence you can have

P×V=mN3d3vrms2×d3 =mNvrms23  P \times V = \dfrac{{mN}}{{3{d^3}}}v_{rms}^2 \times {d^3} \\\ = \dfrac{{mNv_{rms}^2}}{3} \\\

Step 4:
The average kinetic energy of a gas particle is
K=12mvrms2K = \dfrac{1}{2}mv_{rms}^2
Hence, you can rewrite the relation in eq (1) as
PV=23N×12mvrms2 =23NK  PV = \dfrac{2}{3}N \times \dfrac{1}{2}mv_{rms}^2 \\\ = \dfrac{2}{3}NK \\\
Step 5:
Now from ideal gas relation you have
PV=NkbTPV = N{k_b}T
where, kb{k_b} is the universal Boltzmann constant and TT is the temperature of the gas.
Calculate the average translational kinetic energy of a gas particle by using the relation in eq (2)
23NK=NkbT K=32kbT  \dfrac{2}{3}NK = N{k_b}T \\\ \Rightarrow K = \dfrac{3}{2}{k_b}T \\\
Hence, you can see that the average kinetic energy can be solely determined from the temperature TT and the universal Boltzmann constant kb{k_b} .
Final Answer:
The average kinetic energy of the particles of a gas is most closely associated with (B) temperature.

Note: The assumption of elastic collision is to be carefully taken in case of calculation of change of the momentum. The pressure should be calculated on the wall of the container due to the force exerted by the particles. The collisional effects between the molecules are not considered significant as they can be average out to zero in the long run. The other quantities like heat capacity and specific heat can affect the average kinetic energy but not a bit as significant as the temperature as you saw from the derivation.