# heat capacity

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## heat capacity

or## thermal capacity,

ratio of the change in heat**heat,**

nonmechanical energy in transit, associated with differences in temperature between a system and its surroundings or between parts of the same system.

**Measures of Heat**

**.....**Click the link for more information. energy of a unit mass of a substance to the change in temperature

**temperature,**

measure of the relative warmth or coolness of an object. Temperature is measured by means of a thermometer or other instrument having a scale calibrated in units called degrees. The size of a degree depends on the particular temperature scale being used.

**.....**Click the link for more information. of the substance; like its melting point or boiling point, the heat capacity is a characteristic of a substance. The measurement of heat and heat capacity is called calorimetry

**calorimetry**

, measurement of heat and the determination of heat capacity. Heat is evolved in exothermic processes and absorbed in endothermic processes; such processes include chemical reactions, transitions between the states of matter, and the mixing of two substances to form

**.....**Click the link for more information. . In the metric system, heat capacity is often expressed in units of calories

**calorie,**

abbr. cal, unit of heat energy in the metric system. The measurement of heat is called calorimetry. The calorie, or gram calorie, is the quantity of heat required to raise the temperature of 1 gram of pure water 1°C;.

**.....**Click the link for more information. per gram per degree Celsius (cal/g-°C;); in the English system, British thermal units

**British thermal unit,**

abbr. Btu, unit for measuring heat quantity in the customary system of English units of measurement, equal to the amount of heat required to raise the temperature of one pound of water at its maximum density [which occurs at a temperature of 39.

**.....**Click the link for more information. per pound per degree Fahrenheit (Btu/lb-°F;) are often used. Because of the definitions of the calorie and Btu, these two heat capacity units are equivalent; the heat capacity of pure water is 1 cal/g-°C; and 1 Btu/lb-°F;. Other units are used also; for example, the heat capacity of pure water is 4.184 joules/g-°C; and 1.16x10

^{−6}kilowatt-hours/g-°C;. The heat capacity of a system such as a calorimeter refers to the ratio of the change in heat energy of the system as a whole to the change in its temperature and is expressed in such units as calories per degree Celsius. See also specific heat

**specific heat,**

ratio of the heat capacity of a substance to the heat capacity of a reference substance, usually water. Heat capacity is the amount of heat needed to change the temperature of a unit mass 1°.

**.....**Click the link for more information. .

## Heat capacity

The quantity of heat required to raise a unit mass of homogeneous material one unit in temperature along a specified path, provided that during the process no phase or chemical changes occur, is known as the heat capacity of the material in question. Moreover, the path is so restricted that the only work effects are those necessarily done on the surroundings to cause the change to conform to the specified path. The path is usually at either constant pressure or constant volume.

In accordance with the first law of thermodynamics, heat capacity at constant pressure *C*_{p} is equal to the rate of change of enthalpy with temperature at constant pressure ∂*H*/∂*T*)_{p}. Heat capacity at constant volume *C*_{v} is the rate of change of internal energy with temperature at constant volume (∂*U*/∂*T*)_{v}. Moreover, for any material, the first law yields the relation *See* Enthalpy, Internal energy, Thermodynamic principles

*The Great Soviet Encyclopedia*(1979). It might be outdated or ideologically biased.

## Heat Capacity

(or thermal capacity), the quantity of heat absorbed by a substance when its temperature is raised 1 degree. Instantaneous heat capacity is the ratio of the heat absorbed by a substance, upon an infinitesimal change in its temperature, to the change in temperature. The heat capacity per unit mass (in, for example, g or kg) of a substance is called the specific heat. The heat capacity per mole of a substance is known as the molar, mo-lal, or molecular heat capacity.

The quantity of heat absorbed by a substance when a change of state occurs depends not only on the initial and final states—in particular, on their temperature—but also on the means by which the transition between them was accomplished. Accordingly, the heat capacity of a substance depends on the method of heating. A distinction is usually made between the heat capacity at constant volume (*c _{v}*) and the heat capacity at constant pressure (

*c*) depending on whether the volume or pressure, respectively, is held constant during the heating process. In the case of heating at constant pressure, part of the heat provides the energy needed to do the work of expanding the substance, and part goes to increase the internal energy of the substance. For heating at constant volume, all the heat goes to increase the internal energy. Consequently,

_{p}*c*is always greater than

_{p}*c*. For gases that are so rarified that they may be regarded as ideal, the difference in molar heat capacities

_{v}*c*–

_{p}*c*is equal to

_{v}*R*, the universal gas constant, which is equal to 8.314 joules per mole degree Kelvin (J/mol °K), or 1.986 calories per mole degree Celsius (cal/mol °C). In liquids and solids, the difference between

*c*and

_{p}*c*is comparatively small.

_{v}The theoretical calculation of heat capacity—in particular, the calculation of the dependence of the heat capacity on the temperature of the substance—cannot be carried out by means of purely thermodynamic methods and requires application of the methods of statistical mechanics. For gases, the calculation of heat capacity reduces to calculating the average energy of the thermal motion of the individual molecules. This motion consists of the translational and rotational motions of the molecule as a whole and of the vibrational motion of the atoms within the molecule.

According to classical statistics—that is, statistical mechanics based on classical mechanics—each degree of freedom of translational and rotational motion contributes the amount *R*/2 to the molar heat capacity (*c _{v}*) of a gas, and each vibrational degree of freedom contributes the amount

*R*. This principle is called the equipartition of energy. A particle of a monatomic gas has three translational degrees of freedom. Accordingly, the molar heat capacity of the gas should be 3

*R*/2 (that is, about 12.5 J/mol °K, or 3 cal/mol °C), which is in good agreement with experiment. A molecule of a diatomic gas has three translational, two rotational, and one vibrational degree of freedom, and the equipartition law yields the value

*c*= 7

_{v}*R*/2.

Experiment, however, shows that the molar heat capacity of a diatomic gas at ordinary temperatures is actually 5*R*/2. The reason for this discrepancy between theory and experiment is that in calculating the molar heat capacity quantum effects must be taken into account—that is, a statistics based on quantum mechanics must be used. According to quantum mechanics, any system of particles that execute vibrations or rotations (including a gas molecule) can have only certain discrete energy values. If the energy of thermal motion in the system is insufficient to excite vibrations of a certain frequency, then these vibrations do not contribute to the heat capacity of the system; the corresponding degree of freedom is “frozen”—that is, the equipartition law is inapplicable.

The temperature *T* at which the equipartition law is applicable to rotational or vibrational degrees of freedom is determined by the quantum-mechanical relation *T* ≫ *hvlk*, where *v* is the frequency of the vibrations, *h* is Planck’s constant, and *k* is the Boltzmann constant. The intervals between the rotational energy levels of a diatomic molecule (divided by *k*) are just a few degrees and reach a hundred degrees only for such a light molecule as the hydrogen molecule. At ordinary temperatures, the rotational part of the heat capacity of diatomic (and sometimes polyatomic) gases therefore obeys the equipartition law. By contrast, the intervals between vibrational energy levels reach a few thousand degrees. At ordinary temperatures, the equipartition law is consequently inapplicable to the vibrational part of the heat capacity. The calculation of heat capacity on the basis of quantum statistics indicates that the vibrational part of heat capacity decreases rapidly with decreasing temperature and approaches zero. For this reason, even at ordinary temperatures the vibrational part of heat capacity is practically absent, and the molar heat capacity of a diatomic gas is 5*R*/2 instead of 7*R*/2.

At sufficiently low temperatures, heat capacity must in general be calculated by means of quantum statistics. The heat capacity decreases with decreasing temperature and approaches zero as *T* → 0, in accordance with the Nernst heat theorem (the third law of thermodynamics).

In solids (crystalline substances) the thermal motion of the atoms occurs as small vibrations near certain equilibrium positions (lattice points). Each atom thus has three vibrational degrees of freedom. According to the equipartition law, the molar heat capacity of a solid—that is, the heat capacity of the crystal lattice—should be equal to 3*nR*, where *n* is the number of atoms in the molecule. In actuality, however, this value is the limit approached by the molar heat capacity of a solid at high temperatures. The limit is reached at ordinary temperatures in many elements, including the metals, for which *n* = 1 and the Dulong and Petit law applies. It is also reached in some simple compounds, such as NaCl and MnS, for which *n* = 2, and PbCl_{2}, for which *n* = 3. In complex compounds the limit is never actually reached, since melting or decomposition of the substance begins before the limit can be attained.

The quantum theory of the heat capacity of solids was developed by A. Einstein in 1907 and P. Debye in 1912. The theory is based on the quantization of the vibrational motion of the atoms in a crystal. At low temperatures, the specific heat of a solid is proportional to the cube of the absolute temperature; this principle is known as the Debye *T*^{3} law. High and low temperatures can be distinguished through comparison with the parameter characteristic of each individual substance called the characteristic, or Debye, temperature θ* _{D}*. This quantity is determined by the vibration spectrum of the atoms in the substance and thus depends essentially on the crystal structure. Although θ

*is usually of the order of a few hundred °K, it can reach thousands of °K—for example, in diamond (*

_{D}*see*DEBYE TEMPERATURE).

In metals, conduction electrons also make a definite contribution to heat capacity. This part of heat capacity can be calculated by means of Fermi statistics, which electrons obey. The electronic specific heat of a metal is proportional to the absolute temperature. A comparatively small quantity, the electronic contribution to the specific heat of a metal becomes considerable at temperatures close to absolute zero: at temperatures of the order of a few degrees, the specific heat associated with the vibrations of atoms in the crystal lattice is a still smaller quantity.

Table 1. Specific heats of some substances | |
---|---|

Substance | Specific heat (kcal/kg °C) |

Nitrogen ............... | 0.249 |

Hydrogen ............... | 3.42 |

Iron ............... | 0.104 |

Copper ............... | 0.091 |

Aluminum ............... | 0.210 |

Lead ............... | 0.030 |

Quartz ............... | 0.174 |

Ethyl alcohol ............... | 0.547 |

Water ............... | 1.008 |

Table 1 gives the specific heats, in kilocalories per kilogram degree, of some gases, liquids, and solids at a temperature of 0°C and at atmospheric pressure (1 kilocalorie is equal to 4.19 kilojoules).

### REFERENCES

Kikoin, I. K., and A. K. Kikoin.*Molekuliarnaia fizika*. Moscow, 1963.

Landau, L. D., and E. M. Lifshits.

*Statislicheskaia fizika*, 2nd ed. (

*Teoreticheskaia fizika*, vol. 5.) Moscow, 1964.

E. M. LIFSHITS

## heat capacity

[′hēt kə‚pas·əd·ē]## Heat capacity

The quantity of heat required to raise a unit mass of homogeneous material one unit in temperature along a specified path, provided that during the process no phase or chemical changes occur, is known as the heat capacity of the material in question. Moreover, the path is so restricted that the only work effects are those necessarily done on the surroundings to cause the change to conform to the specified path. The path is usually at either constant pressure or constant volume.

In accordance with the first law of thermodynamics, heat capacity at constant pressure *C*_{p} is equal to the rate of change of enthalpy with temperature at constant pressure. Heat capacity at constant volume *C*_{v} is the rate of change of internal energy with temperature at constant volume. Moreover, for any material, the first law yields the relation

*See* Enthalpy, **I<SCP>nternal energy</SCP>**, **T<SCP>hermodynamic principles</SCP>.**