techniques for approximating the international temperature ... - BIPM

techniques for approximating the international temperature ... - BIPM techniques for approximating the international temperature ... - BIPM

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10 2. Uniform-Temperature Enclosures Calibration of thermometers requires uniform-temperature enclosures. All of the apparatuses described here to produce such enclosures may be constructed in the laboratory, or, alternatively, may be obtained commercially. The latter tend to be more costly and to provide poorer, although adequate, uniformity. For comparison calibrations, the uncalibrated thermometer and the laboratory standard are mounted in such a way as to be in good mutual thermal contact, as in a solid metal block or a stirred liquid. Significant errors can be avoided by proper attention to immersion depths, heat transfer along thermometer leads, thermal time lags, thermometer self-heating, temperature differences within the enclosure, radiation exchange with the environment, and so on. The type of enclosure used depends upon the temperature range involved. 2.1 1 K TO 300 K Several apparatuses that serve for the calibration of thermometers have been described. The temperature stability and uniformity of the apparatuses depend upon both their thermal design and the quality of the associated temperature controller. One that is simple, that has worked extremely well for calibrating capsule PRTs, and that can be used with germanium (Ge) or rhodium-iron (RhFe) resistance thermometers is shown in Fig. 2.1. A small copper block with holes for four thermometers is surrounded by two concentric copper radiation shields in an insulated container which is open at the bottom. The container hangs by a thin-walled metal tube in a liquid helium dewar. To prevent heat transfer along the thermometer leads, the latter pass through insulated holes in the copper block and one of the shields. Heaters are wound on both the block and the shields, and the temperature difference between them is measured with differential thermocouples. The block is cooled to liquid helium temperatures and the liquid is then blown out of the insulated container, leaving helium gas at atmospheric pressure therein. The liquid helium remaining in the dewar provides the necessary cooling. The block is heated to, and then maintained at, each desired temperature in turn, the shield temperatures being adjusted to be that of the block by a servo-control. The apparatus requires no vacuum feed-throughs for the leads and the thermometers rapidly reach equilibrium as a result of the good thermal contact between the block and the thermometer provided by the helium gas. With this system a PRT can be calibrated to within 1 mK.

11 Fig. 2.1: One form of apparatus used at NRC for calibration of resistance thermometers from 4.2 K to 273.15 K: A, metal cover; B, copper shields; C, copper block; D, expanded polystyrene; E, capsule PRT; F, liquid helium. An alternative procedure that is also widely used is to place the thermometers in a copper block that is enclosed within suitable radiation shields in an evacuated cryostat as shown in Fig. 2.2 (see, for example, Rusby et al. (1972), Compton and Ward (1975), or Besley and Kemp (1977)). Details of operation are given in the suggested references. It is sometimes useful to design the cryostat in a modular way to allow for the use of a single apparatus for different experiments. This may be facilitated by the incorporation of a cylindrical re-entrant well in the tube connecting the cryostat chamber to the part of the apparatus that is at room temperature. In this way, different modules, designed for different experiments, can be interchanged from the top flange, without one's having to disassemble the cryostat itself [see Pavese (1981 )]. For temperatures above 4 K, it is also possible to use closed-cycle refrigerators, so avoiding conventional liquid refrigerants and allowing convenient and faster operation. The thermal design of measuring modules for such a system is similar to that of a flow cryostat (Fig. 2.3) [Blanke and Thomas (1979)], but care must be taken to prevent mechanical - vibrations from adversely affecting the thermometer.

10<br />

2. Uni<strong>for</strong>m-Temperature Enclosures<br />

Calibration of <strong>the</strong>rmometers requires uni<strong>for</strong>m-<strong>temperature</strong> enclosures. All of <strong>the</strong><br />

apparatuses described here to produce such enclosures may be constructed in <strong>the</strong><br />

laboratory, or, alternatively, may be obtained commercially. The latter tend to be more costly<br />

and to provide poorer, although adequate, uni<strong>for</strong>mity. For comparison calibrations, <strong>the</strong><br />

uncalibrated <strong>the</strong>rmometer and <strong>the</strong> laboratory standard are mounted in such a way as to be in<br />

good mutual <strong>the</strong>rmal contact, as in a solid metal block or a stirred liquid. Significant errors<br />

can be avoided by proper attention to immersion depths, heat transfer along <strong>the</strong>rmometer<br />

leads, <strong>the</strong>rmal time lags, <strong>the</strong>rmometer self-heating, <strong>temperature</strong> differences within <strong>the</strong><br />

enclosure, radiation exchange with <strong>the</strong> environment, and so on. The type of enclosure used<br />

depends upon <strong>the</strong> <strong>temperature</strong> range involved.<br />

2.1 1 K TO 300 K<br />

Several apparatuses that serve <strong>for</strong> <strong>the</strong> calibration of <strong>the</strong>rmometers have been<br />

described. The <strong>temperature</strong> stability and uni<strong>for</strong>mity of <strong>the</strong> apparatuses depend upon both<br />

<strong>the</strong>ir <strong>the</strong>rmal design and <strong>the</strong> quality of <strong>the</strong> associated <strong>temperature</strong> controller. One that is<br />

simple, that has worked extremely well <strong>for</strong> calibrating capsule PRTs, and that can be used<br />

with germanium (Ge) or rhodium-iron (RhFe) resistance <strong>the</strong>rmometers is shown in Fig. 2.1.<br />

A small copper block with holes <strong>for</strong> four <strong>the</strong>rmometers is surrounded by two concentric<br />

copper radiation shields in an insulated container which is open at <strong>the</strong> bottom. The container<br />

hangs by a thin-walled metal tube in a liquid helium dewar. To prevent heat transfer along<br />

<strong>the</strong> <strong>the</strong>rmometer leads, <strong>the</strong> latter pass through insulated holes in <strong>the</strong> copper block and one<br />

of <strong>the</strong> shields. Heaters are wound on both <strong>the</strong> block and <strong>the</strong> shields, and <strong>the</strong> <strong>temperature</strong><br />

difference between <strong>the</strong>m is measured with differential <strong>the</strong>rmocouples. The block is cooled to<br />

liquid helium <strong>temperature</strong>s and <strong>the</strong> liquid is <strong>the</strong>n blown out of <strong>the</strong> insulated container, leaving<br />

helium gas at atmospheric pressure <strong>the</strong>rein. The liquid helium remaining in <strong>the</strong> dewar<br />

provides <strong>the</strong> necessary cooling. The block is heated to, and <strong>the</strong>n maintained at, each<br />

desired <strong>temperature</strong> in turn, <strong>the</strong> shield <strong>temperature</strong>s being adjusted to be that of <strong>the</strong> block by<br />

a servo-control. The apparatus requires no vacuum feed-throughs <strong>for</strong> <strong>the</strong> leads and <strong>the</strong><br />

<strong>the</strong>rmometers rapidly reach equilibrium as a result of <strong>the</strong> good <strong>the</strong>rmal contact between <strong>the</strong><br />

block and <strong>the</strong> <strong>the</strong>rmometer provided by <strong>the</strong> helium gas. With this system a PRT can be<br />

calibrated to within 1 mK.

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