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                                                                      ∗
                                          TABLE 19.4  Fixed Points Used in ITS 90
                                          Triple point of hydrogen          13.8033 K
                                          Triple point of neon              24.5561 K
                                          Triple point of oxygen            54.3584 K
                                          Triple point of argon             83.8058 K
                                          Triple point of mercury          234.3156 K
                                          Triple point of water            273.16 K
                                          Melting point of gallium         302.9146 K
                                          Freezing point of indium         429.7485 K
                                          Freezing point of tin            505.078 K
                                          Freezing point of zinc           692.677 K
                                          Freezing point of aluminum       933.573 K
                                          Freezing point of silver        1234.93 K
                                          Freezing point of gold          1337.33 K
                                          Freezing point of copper        1357.77 K
                                            ∗
                                            Magnum (1990) includes the full definition of these points.
                       the discussion of temperature measuring techniques presented here. While this definition may help us
                       understand the concept of temperature, it does not help us assign a numerical value to temperature or
                       provide us with a convenient method for measuring temperature. The zeroth law of thermodynamics,
                       formulated in 1931 more than half a century after the first and second laws, lays the foundation for all
                       temperature measurement. It states that if two bodies are in thermal equilibrium with a third body, they
                       are also in thermal equilibrium with each other. By replacing the third body with a thermometer, we can
                       state that two bodies are in thermal equilibrium if both have the same temperature reading even if they
                       are not in contact.
                         The zeroth law does not enable the assignment of a numerical value for temperature. For that we must
                       refer to a standard scale of temperature. Two absolute temperature scales are defined such that the
                       temperature at zero corresponds to the theoretical state of no molecular movement of the substance. This
                       leads to the Kelvin scale for the SI system and the Rankine scale for the English system. There are other
                       two-point scales derived by identifying two arbitrary defining points for temperature. These are usually
                       defined as the temperature at which a pure substance undergoes a change in phase. Familiar defining
                       points are the freezing and boiling point of water for 0°C and 100°C, respectively. A wide range of
                       such phase changes, many of them triple points where all three phases are in equilibrium, have been
                       accepted as the defining points of the International Practical Temperature Scale of 1990 (ITS 90 ) shown
                       in Table 19.4. These can be used directly as calibration points for temperature monitors as long as the
                       substances are pure and the other conditions, such as pressure, which are included in the defining points
                       are met. Within the ITS 90  guidelines are standard means of interpolating temperatures between the defined
                       points. For example, platinum resistors are used in the range from 13.8 to 1235 K. The resistance is fitted
                       to the temperature through a higher-order polynomial that may be simplified for more limited ranges
                       between defined temperature points. The difference between a linear interpolation of resistance between
                       the defined points and the higher-order polynomial interpolation never exceeds 2 mK (Magnum and
                       Furukawa, 1990).
                         Another complication that is encountered in any discussion of temperature measurement is the fact
                       that temperature is an intrinsic rather than an extrinsic property. Thus, temperature can not be added,
                       subtracted, and divided in the same way that measured extrinsic properties such as length or voltage can
                       be manipulated.
                         Any property that changes predictably in response to temperature can be used in a temperature sensor.
                       The discussion of temperature measuring devices given here subdivides the devices based on the mea-
                       suring principle. Discussion will begin with a series of thermometers that rely upon the differential
                       expansion coefficients of the materials, be they solid, liquid, or gas. Mercury thermometers, perhaps the
                       most well known and widely used of all temperature measuring devices, belong to this category. We will
                       then move on to devices that rely upon phase change. Next we will discuss electrical temperature sensors
                       and transducers. Included in this category are thermocouples, RTDs, and thermistors, as well as integrated

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