Internal Energy of an Ideal Gas Formula

Physics · Kinetic Theory · NEET

The internal energy of an ideal gas is U = (f/2) nRT, where f is the degrees of freedom, n is the number of moles, R is the gas constant and T is the absolute temperature. For an ideal gas there are no intermolecular forces, so U is purely kinetic and depends only on temperature, not on pressure or volume. Memory hook: "f over 2, times nRT" — count the degrees of freedom (3 for monatomic, 5 for diatomic) and the rest is fixed.
Internal Energy of an Ideal Gas: U = (f/2) nRTMonatomic (He, Ar)f = 3U = (3/2) nRTDiatomic (O2, N2)f = 5U = (5/2) nRTPolyatomic (rigid)f = 6U = 3 nRTMore degrees of freedom means more internal energy at the same temperature T
Internal energy U = (f/2) nRT scales with degrees of freedom: monatomic gases store (3/2) nRT, diatomic (5/2) nRT and rigid polyatomic 3 nRT at the same temperature.

Your doubts, answered

Does the internal energy of an ideal gas depend on pressure or volume?

No. For an ideal gas, U depends only on the absolute temperature T. The formula U = (f/2) nRT has no P or V in it. If you compress a gas but keep T the same (isothermal), U does not change. This is why in an isothermal process the change in internal energy is zero. Pressure and volume can change, but as long as T is fixed, U is fixed.

Why is the internal energy of an ideal gas purely kinetic energy?

An ideal gas is assumed to have no forces between molecules except during collisions. Internal energy is the sum of molecular kinetic energy plus molecular potential energy. Since there are no intermolecular forces, the potential energy part is zero. So only kinetic energy is left, and kinetic energy depends only on temperature. That is why U is a function of T alone for an ideal gas.

What is the internal energy of a monatomic gas versus a diatomic gas?

A monatomic gas (like He, Ar) has f = 3 (three translational degrees of freedom), so U = (3/2) nRT. A diatomic gas (like O2, N2, H2) treated as a rigid rotator has f = 5 (3 translational + 2 rotational), so U = (5/2) nRT. A polyatomic gas has f = 6 (3 translational + 3 rotational) for the rigid case, giving U = 3 nRT. More degrees of freedom means more internal energy at the same temperature.

How does U = (f/2) nRT come from the law of equipartition of energy?

Equipartition says each degree of freedom carries an average energy of (1/2) kB T per molecule. A molecule with f degrees of freedom has average energy (f/2) kB T. One mole has NA molecules, so energy per mole is (f/2) NA kB T = (f/2) RT, because NA kB = R. For n moles, U = (f/2) nRT.

What is the change in internal energy when temperature changes?

Since U = (f/2) nRT, the change is ΔU = (f/2) nR ΔT. This depends only on the temperature change, not on the path taken. Whether the process is isobaric, isochoric or any other, if the temperature rises by the same ΔT, ΔU is the same. For example, for a monatomic gas ΔU = (3/2) nR ΔT.

⚠️ The NEET trap
In an isothermal expansion the gas expands and does work, so students assume its internal energy increases.
In an isothermal process T is constant, so ΔU = 0 for an ideal gas. The heat supplied all goes into work done by the gas; internal energy does not change.
🧠 For an ideal gas, U tracks temperature only. No temperature change means no internal energy change, no matter how V or P move.

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Frequently asked

What is the formula for internal energy of an ideal gas?

U = (f/2) nRT, where f is degrees of freedom, n is moles, R is the gas constant and T is absolute temperature in kelvin.

Is internal energy of an ideal gas a state function?

Yes. It depends only on the current state (temperature), not on how the gas reached that state. That is why ΔU over a cyclic process is zero.

What is the internal energy per mole of a monatomic ideal gas?

For one mole of a monatomic gas, U = (3/2) RT, since it has 3 translational degrees of freedom.

Does internal energy include potential energy for an ideal gas?

No. An ideal gas has no intermolecular forces, so molecular potential energy is zero. The internal energy is entirely molecular kinetic energy.

How is internal energy related to specific heat at constant volume?

Since ΔU = (f/2) nR ΔT and ΔU = n Cv ΔT at constant volume, we get Cv = (f/2) R. This links internal energy directly to the molar specific heat Cv.