1.7.10 · D1Thermodynamics

Foundations — Internal energy of ideal gas U = (f - 2)nRT

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Before you can trust the parent formula, you must be able to read every letter in it without hesitation. This page builds each symbol from absolute zero, in an order where each one leans only on the ones before it. Nothing is assumed.


0 — The mental picture we keep returning to

Figure — Internal energy of ideal gas U = (f - 2)nRT

Picture a sealed box full of tiny hard balls, zooming in every direction, bouncing off the walls and each other. That is our gas. Everything below is a way of counting or measuring something about this swarm. Keep this picture in your head — every symbol points back to it.


1 — Counting the particles: , ,

That number is enormous (trillions of trillions), so counting one-by-one is hopeless. Instead we count in bundles called moles.


2 — Measuring the swarm's state: , ,

These three are what you could measure from outside the box, without seeing individual molecules.

Figure — Internal energy of ideal gas U = (f - 2)nRT

3 — The universal glue: the ideal gas law and its constants ,

Now connect the outside measurements () to the counts (). This link is the Ideal gas law.

Two constants appear. They are the same idea at two counting scales.


4 — The energy we actually want: kinetic energy and

Different molecules move at different speeds, so we need an average.

This is why the kinetic-theory result the parent quotes, puts (not ) on the right: it is really a statement about total kinetic energy dressed up as a pressure. See Kinetic theory of gases.


5 — The counting of "ways to move": degrees of freedom

Figure — Internal energy of ideal gas U = (f - 2)nRT

A single point-like atom can move along three independent directions — left/right, forward/back, up/down. That is 3 translational degrees of freedom. A dumbbell-shaped diatomic molecule can also tumble end-over-end about two axes, adding 2 rotational degrees of freedom, giving . See Degrees of freedom for the full count.


6 — The half: where comes from

The in the formula is really . The is the energy nature puts into each channel per molecule: . Multiply by channels → per molecule → multiply by molecules and swap . Every piece is now a symbol you have met.


7 — Symbols that ride along: , , ,


Prerequisite map

Counting N n and NA

Ideal gas law PV = nRT

State variables P V T

Bridge N kB = n R

Kinetic theory and mean square speed

Translational KE per molecule

Equipartition half kB T per DOF

Degrees of freedom f

Energy per molecule = f over 2 kB T

U = f over 2 n R T

First law delta U = Q minus W


Equipment checklist

Cover the right side and test yourself before moving to the derivation page.

means
the plain count of individual molecules in the box.
means
the number of moles = bundles of molecules.
means
Avogadro's number , molecules per mole, with .
(in kelvin) physically measures
the average kinetic energy of random molecular motion.
Why must be in kelvin
only kelvin is proportional to actual molecular energy and starts at absolute zero.
The ideal gas law in molecule form
.
The bridge relation between the two constants
, equivalently .
pairs with
the molecule count ; pairs with the mole count .
Why we average and not
energy depends on , and squaring stops opposite directions from cancelling.
A degree of freedom is
one independent way a molecule can store energy of motion.
for monatomic / diatomic
3 / 5.
Why appears in
energy shares equally into every channel, so more channels store more energy.
means
final internal energy minus initial internal energy.
Relation of , ,
(first law).

Connections