Number of mtermed=atΒ’ coohng stattons, N Ftg.3 Minimum self-sufficient hod-off rate for various numbers of intermediate heat exchangers; rn/v--~ oo gwen by (13)
Automatic temperature control of a superconducting bolometer
β Scribed by I.A. Khrebtov; N.M. Gopshtein; G.A. Zaitsev
- Publisher
- Elsevier Science
- Year
- 1972
- Tongue
- English
- Weight
- 180 KB
- Volume
- 12
- Category
- Article
- ISSN
- 0011-2275
No coin nor oath required. For personal study only.
β¦ Synopsis
exhibited very large boil-offs at currents beyond 600 A. The resistance ratio of the copper, measured at 290 K and 4.2 K was 398. This corresponds to the second column of Table . The temperature distributions for the same purity copper calculated on the basis of equations 8 and 3 are displayed as curves A and B respectively in Fig. . For reference, the electrical resistivity, p, and the product WT, are also shown (curves C and D) in reduced coordinates as functions of temperature. The value of the series resistor required to keep the temperature distribution between the two limiting curves was calculated from (12). When this was installed currents up to 1 200 A produced only moderate boil-offs.
In conclusion, it would seem that the installation of a resistor below the liquid level of a helium bath has definite advantages if high currents are passed intermittently. It also provides a simple method of uprating existing optimized lead assemblies and it may well offer a useful additional control in continuously operating high current cryogenic systems.
π SIMILAR VOLUMES
A simple temperature controller which does not involve compficated electronic equipment is described. It provides flexible, accurate temperature control for a wide range of cryogenic systems and laboratory experiments. The controller can be operated in several different modes to achieve minimum star
A viscoelastic body which undergoes a thermomechanical process is considered. The evolution of the state variables, i.e., the displacement and temperature "elds, is described by a coupled hyperbolic}parabolic integrodi!erential system. The heat #ux through a portion of the boundary is controlled aut