• Pixel-art sticker of Equipa, personifying Equipartition Theorem, with the caption "Everyone Gets Half Kt."

IndexHeat & EntropySticker

Equipa

Equipartition Theorem Physics

\[\langle E \rangle = \tfrac{1}{2} k_B T\]
Regular price $4.99 USD
Regular price Sale price $4.99 USD
Sale Sold out

Meet Equipa, who shares energy fairly in classical thermal equilibrium: each quadratic degree of freedom gets an average of ½kBT, where kB is the Boltzmann constant. The rule fails where quantum effects freeze modes out. Pixel-art kiss-cut sticker in 2, 3, 4 and 6 inches; equation, symbols and sources in the physics panel below.

Size
Surface

Flat $6 shipping worldwideMade to order, ships in 2–5 business days

Details

Size3″ × 3″

3″ × 3″ kiss-cut sticker.

Shipping

Flat $6 shipping on every order, worldwide, whatever's in it.

Delivery times & where we ship

Returns & replacements21 days

Every item is printed to order, so we can’t accept returns or exchanges for change of mind, or if you ordered the wrong size or colour.

Print defect, misprint, damage or the wrong item? We’ll send a free replacement, or a refund if you prefer. Report it within 21 days of delivery with a photo; no need to send it back.

Full refund & replacement policy

The physics

Meet Equipa, who shares energy out fairly: the same average slice for every way a molecule can move.

In a gas in thermal equilibrium, energy is constantly passed around in collisions. The equipartition theorem of classical physics says that each 'quadratic' degree of freedom, meaning each term in the energy that goes as a square of a speed or a position, gets on average ½k_BT of energy.

A helium atom can move in three directions, so its average kinetic energy is 3/2 k_BT. At room temperature, 300 K, that is about 6.2×10⁻²¹ joules. A nitrogen molecule can also rotate about two axes, giving it 5/2 k_BT, which is why the molar heat capacity of air is larger than that of helium.

Equipartition explains measured heat capacities of many gases and the Dulong–Petit value for solids at room temperature.

It also fails, and the failures mattered. Molecular vibrations hold far less energy than equipartition predicts at room temperature, and solids' heat capacities fall at low temperature. Explaining these 'frozen out' modes was one of the clues that led to quantum theory.

Equations

\[\langle E \rangle = \tfrac{1}{2} k_B T\]
Symbols
SymbolMeaningUnit
\(\langle E\rangle\) average energy per quadratic degree of freedom \(\mathrm{J}\)
\(k_B\) Boltzmann constant \(\mathrm{J/K}\)
\(T\) absolute temperature \(\mathrm{K}\)