PROOF:-
As we know from the kinetic theory of gases, the macroscopic pressure exerted by an ideal gas is given by the relation:
Since gas density is defined as total mass divided by internal volume ($\rho = \frac{mN}{V}$), we can rewrite the equation as:
Also, from the macroscopic ideal gas equation for an ideal state, we know that:
Since the number of moles is $n = \frac{N}{N_A}$ (where $N$ is total molecules and $N_A$ is Avogadro's number):
Substituting Boltzmann's constant ($k_B = \frac{R}{N_A}$) gives:
Comparing equation (i) and equation (ii), we get:
Canceling the total number of molecules ($N$) from both sides yields:
To explicitly reveal the kinetic energy structural term, we multiply and divide the left side by "$2$":
Since the average translational kinetic energy of a single molecule is defined as $\text{K.E.}_{\text{avg}} = \frac{1}{2}m\overline{v^2}$, we can write:
Since $\frac{3}{2}$ and $k_B$ are fundamental physical constants, the equation simplifies to:
Hence proved that "The average Translational K.E. of a gas molecule is directly proportional to the absolute temperature."
EXPRESSION FOR KINETIC ENERGY PER MOLE
To determine the macroscopic kinetic energy of one complete mole of gas ($E_m$), we multiply the single-molecule energy equation (iii) by Avogadro's number ($N_A$):
Since $N_A k_B = R$ (the Universal Gas Constant), the kinetic expression for one mole of gas is:
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