Editing Thermodynamics (section)

== Instrumentation ==
There are two types of [[thermodynamic instruments]], the meter and the reservoir. A thermodynamic meter is any device which measures any parameter of a [[thermodynamic system]]. In some cases, the thermodynamic parameter is actually defined in terms of an idealized measuring instrument. For example, the [[zeroth law of thermodynamics|zeroth law]] states that if two bodies are in thermal equilibrium with a third body, they are also in thermal equilibrium with each other. This principle, as noted by [[James Clerk Maxwell|James Maxwell]] in 1872, asserts that it is possible to measure temperature. An idealized [[thermometer]] is a sample of an ideal gas at constant pressure. From the [[ideal gas law]] ''pV=nRT'', the volume of such a sample can be used as an indicator of temperature; in this manner it defines temperature. Although pressure is defined mechanically, a pressure-measuring device, called a [[barometer]] may also be constructed from a sample of an ideal gas held at a constant temperature. A [[calorimeter]] is a device which is used to measure and define the internal energy of a system.

A thermodynamic reservoir is a system which is so large that its state parameters are not appreciably altered when it is brought into contact with the system of interest. When the reservoir is brought into contact with the system, the system is brought into equilibrium with the reservoir. For example, a pressure reservoir is a system at a particular pressure, which imposes that pressure upon the system to which it is mechanically connected. The Earth's atmosphere is often used as a pressure reservoir. The ocean can act as temperature reservoir when used to cool power plants.