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To prove this, we will have to use 3 equations, 2 of them related to ideal gases:

(i) pV = nRT

(ii) p = 1/3 d <c2>

(iii) Ek = 1/2 mv2

First of all, an ideal gas has no intermolecular forces. Thus, its molecules have no potential energy.

The internal energy of any system can be defined as the sum of the randomly distributed microscopic potential energy and kinetic energy of the molecules of the system.

It is thus evidently clear that the internal energy of an ideal gas is entirely kinetic. (Ep being zero)

So, U = 1/2 m <c2> (for an ideal gas)

From (i) and (ii), <c2> = 3p/d = 3pV/m = 3nRT/m (d= m/V)

Substituting in the appropriate equation, we get:

U = 1/2 m (3nRT/m)

U = 3/2 nRT

From the above equation, it can be concluded that for a fixed mass of an ideal gas, internal energy is proportional to the thermodynamic temperature. (fixed mass such that n is constant)

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