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Size & fitS–5XL

Unisex heavy cotton (Gildan 5000), classic fit.

Unisex tee size chart, inches
SizeWidthLengthSleeve
S182815.1
M202916.5
L223018
XL243119.5
2XL263221
3XL283322.4
4XL303423.7
5XL323525

Measurements in inches, ±1.5 in tolerance.

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The physics

Entropy Warden keeps one ledger, and it has only one column.

In 1865 Rudolf Clausius needed a name for a quantity he had tracked for over a decade. He built it from the Greek word for transformation and made it sound like energy on purpose, because he thought the two belonged together. The definition is the first line on this page: when a body takes in a small amount of heat reversibly, its entropy rises by that heat divided by the absolute temperature at which it arrives.

That division is the whole trick. Let one joule of heat leak from a block at 400 kelvin into a block at 300 kelvin. The hot block loses 1/400 of a joule per kelvin. The cold block gains 1/300. The cold block gains more than the hot one lost, so the total goes up, by about 0.00083 joules per kelvin. Run it backward and the total would fall. Clausius had already put the rule into words: heat cannot of itself pass from a colder to a hotter body. The second line, entropy of an isolated system never decreasing, is that sentence turned into arithmetic.

Note the words "of itself". A refrigerator moves heat uphill all day. It does it by dumping that heat, plus the work drawn from the wall socket, into your kitchen, and the kitchen's entropy rises by more than the inside of the fridge loses. Local order is allowed. It is paid for elsewhere, always in full.

Clausius ended the 1865 paper with two sentences: the energy of the world is constant; the entropy of the world tends toward a maximum. The first is a conservation law. The second is the Warden's job description.

She stops nothing. She only writes it down, and nothing she writes is ever erased.

Equations

\[dS = \frac{\delta Q_{\text{rev}}}{T}\]
\[\Delta S_{\text{isolated}} \ge 0\]
Symbols
SymbolMeaningUnit
\(S\) entropy \(\mathrm{J/K}\)
\(\delta Q_{\text{rev}}\) heat exchanged reversibly \(\mathrm{J}\)
\(T\) absolute temperature \(\mathrm{K}\)
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