Comparison of the Fahrenheit, Celsius, and Kelvin scales.
Temperature is the quantity that tells how warm or cold an object is with respect to some standard. It is a measure of the average kinetic energy of the molecules or atoms in an object. The temperature of matter is expressed by a number that corresponds to the degree of hotness on a chosen scale: Celsius (°C), Fahrenheit (°F), or kelvin (K) and is measured quantitatively by thermometers.
In most laboratory work, temperature is expressed in degrees Celsius, named after the eighteenth century Swedish astronomer Anders Celsius. On the Celsius scale, zero is assigned to the temperature at which water freezes, and 100 is given to the boiling point of water. The Celsius scale is the same as the centigrade scale.
The United States uses the Fahrenheit scale to express temperatures. In this scale, the value 32 is assigned to the freezing point of water and 212 to its boiling point. Conversion to the Fahrenheit scale from Celsius is through the formula: degrees Celsius = 5/9 × (degrees Fahrenheit - 32).
Scientists also used the kelvin scale, named after the British scientist Lord Kelvin (William Thomson). On this scale, zero is assigned to absolute zero – the lowest possible temperature. At absolute zero, a substance has no kinetic energy. Absolute zero corresponds to -273° on the Celsius scale. The absolute temperature scale, unlike the other temperature scales, is not arbitrary; it is defined with an ideal reversible heat engine working on a Carnot cycle between two temperatures T1 and T2. If Q1 is the heat received at the higher temperature T1, and Q2 the heat lost at the lower temperature T2, the T1/T2 is defined equal to Q1/Q2. Such absolute temperature is independent of the properties of particular substances, and is a basic thermodynamic function, arising out of the zeroth law.
Temperature and heat
Temperature is an intensive property, unlike heat, which is an extensive property – that is, the temperature of a body is independent of its mass or nature; it is thus only indirectly related to the heat content (internal energy) of the body. Heat flows always from a higher temperature to a lower. On the molecular scale, temperature may be defined in terms of the statistical distribution of the kinetic energy of the molecules.
Forms of temperature
In radio astronomy, antenna temperature is a measure of the power per unit bandwidth (p) of the signal received by an antenna after losses in the detector system. It is defined as p/k, where k is Boltzmann's constant.
In an ideal, loss-free radio telescope, the antenna temperature is equal to the brightness temperature if the intensity of the received radiation is constant within the main lobe. If the angular dimension of the source is small compared to the main lobe, the antenna temperature is equal to the brightness temperature multiplied by the ratio of the solid angle subtended by the source to the effective solid angle of the antenna.
Color temperature is the temperature of a blackbody that has the same color index as a given star.
For a ferromagnetic material, the Curie temperature (TC) is the temperature above which the material becomes paramagnetic. For iron the Curie temperature is 760°C; for nickel it is 356°C. Also known as the Curie point, it is named after the French physicist Pierre Curie (1859–1906).
Electron temperature is the temperature determined by the mean kinetic energy of free electrons in a plasma; also known as the kinetic temperature. Inside stars, electron temperature is likely to match the temperature as measured by other methods, but in the rarefied environment of a nebula or the outer atmospheres of stars, it may be quite different.
The ionization temperature is the temperature of a gas or plasma derived from the relative numbers of neutral atoms and ions. Specifically, it is the temperature for which the Saha equations would predict these relative numbers, assuming the atoms and ions are in thermodynamic equilibrium.
Kinetic temperature is the temperature of a gas defined in terms of the average kinetic energy of its atoms or molecules. It is given by:
T = 2/3 1/k avg(½ mv 2)
where T is the kinetic temperature, k is Boltzmann's constant, m is the particle mass, and v is the particle velocity. In thermal equilibrium, values of kinetic temperature correspond well with those of other measures of temperature, such as effective temperature; otherwise, they may bear little resemblance.
The radiation temperature is the surface temperature of an object in space, calculated assuming that it behaves as a blackbody. It is the same as the effective temperature but is usually measured over a narrow region of the electromagnetic spectrum, such as the visible range.
Spin temperature is a way of measuring the temperature of neutral hydrogen (HI) in space in terms of the relative populations of its two possible spin states – parallel (electron and proton spins aligned) and antiparallel (spins opposed). The spin temperature of an HI region is the temperature at which its observed ratio of parallel to antiparallel spins would occur if the gas were in thermal equilibrium. It differs from the kinetic temperature at low densities, where the spin temperature is raised by the tendency of resonant scattering of Lyman-alpha photons to equalize the occupation probabilities in the two spin states.