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Chemistry · Ch 6 — Thermodynamics

The general case

6.1.4(c)

The general case

The general case

Now consider the general case in which a change of state is brought about both by doing work and by transferring heat. The change in internal energy for this case is:

ΔU=q+w(5.1)\Delta U = q + w \qquad(5.1)

For a given change in state, qq and ww can vary depending on how the change is carried out. However, the sum q+w=ΔUq + w = \Delta U depends only on the initial and final states. It is independent of the path taken.

If there is no transfer of energy as heat or as work (an isolated system), then w=0w = 0 and q=0q = 0, so ΔU=0\Delta U = 0.

Important

Equation (5.1), ΔU=q+w\Delta U = q + w, is the mathematical statement of the first law of thermodynamics, which states: The energy of an isolated system is constant. This is commonly known as the law of conservation of energy — energy can neither be created nor destroyed. …