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Chemistry · Ch 3 — Thermodynamics

Heat Capacity

3.2.2(c)

Heat Capacity

Heat Capacity

When heat is transferred to a system, the temperature of the system rises. The increase in temperature is proportional to the amount of heat transferred:

q∝ΔTq \propto \Delta T

The constant of proportionality depends on the size, composition, and nature of the system. We write:

q=CΔTq = C\Delta T

where CC is called the heat capacity of the system. Heat capacity tells us how much heat is needed to raise the temperature of the system by one degree (either 1∘C1^\circ\text{C} or 1 K1\ \text{K}). When CC is large, a given amount of heat produces only a small temperature rise. Water, for example, has a large heat capacity — a lot of energy is needed to raise its temperature.

Heat capacity is an extensive property — it depends on how much substance is present. Two related intensive quantities are defined:

Molar heat capacity, CmC_m, is the heat capacity for one mole of the substance:

Cm=CnC_m = \frac{C}{n}

It is the quantity of heat needed to raise the temperature of one mole of the substance by one degree celsius (or one kelvin).

Specific heat capacity (often called simply specific heat), cc, is the quantity of heat required to raise the temperature of one unit mass of a substance by one degree celsius (or one kelvin). …