Thermal equilibrium, internal energy, heat and work · Physics Class 11–12 | StemPy Lab
Course 11.1·Lesson 1 of 3
Thermal equilibrium, internal energy, heat and work
Bodies in contact reach thermal equilibrium at one temperature (the zeroth law). A body's internal energy is the energy of its molecules; for an ideal gas it depends only on temperature, U=2fnRT
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Thermal equilibrium
Put a cold metal block into warm water. Heat flows until both reach one temperature, and then nothing more changes: they are in thermal equilibrium.
The zeroth law: if A and B are each in equilibrium with C, they are in equilibrium with each other. That is why a thermometer (C) can compare A and B: equal readings mean equal temperatures.
Internal energy
Every body holds energy in its molecules: their motion, their spinning, and the pull between them. This is its internal energy, U.
For an ideal gas the molecules do not pull on each other, so U is all motion energy, and it depends only on the temperature. Each way a molecule can move holds 21kBT on average, so
U=2fnRT
with f=3 for a monatomic gas (moving along x, y and z) and f=5 for a diatomic gas (two ways of turning as well).
You should find that doubling the temperature doubles the internal energy, and that a diatomic gas holds 35 times as much as a monatomic gas at the same temperature.
Heat and work
Energy can get into or out of a gas in two ways.
Heat, Q: energy that flows because of a difference of temperature.
Work, W: energy passed by a force moving something, such as a gas pushing a piston.
Neither is something a body has. A body has internal energy; heat and work are energy on the move.
A graph of pressure against volume. Two points are marked, A at the left and B at the right. Three different paths join them. The top path first expands at a high pressure and then falls in pressure at a constant volume. The straight path in the middle goes directly from A to B. The bottom path first falls in pressure at a constant volume and then expands at a low pressure. The area under each path is shaded and is different for each path, so the work done depends on the path. The internal energy at A and at B is the same for all three paths.
Watch out. Temperature is not internal energy. A bath at 40∘C holds far more internal energy than a cup at 40∘C.
A worked example
Find the internal energy of 2.0 mol of helium and of 2.0 mol of nitrogen, both at 300K.