By J. Bass (auth.), K.-H. Hellwege, J. L. Olsen (eds.)
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Additional resources for Electrical Resistivity, Thermoelectrical Power and Optical Properties
6,. 25 77K 0 100 200 300 600 500 kbor 700 PFig. 25. Ho. Resistance at 77, 197, 296K vs. pressure [64Sta 11. ) In (tet, pc). See also [52Br 1, 61 Ba 11. Table 45. In [Sl Br 11. Table 44. In. Quantity Value T Ref. 5,. 0000 5 Fig. 26. In. Pressure coefficient of the ideal resistivity vs. temperature [66Go 11. F t -30 0 50 100 150 I- 200 250 K 300 Table 48. Ir [SlBrl]. 39 -20 Ref. 32 5O 40-6 0 Table 47. Ir. Quantity 2; bar-’ a -10 F: 0 2 Ir (fee, PC). See also [52Br 1). 9727, 20 25 30 T “C 10m5bar- ’ 0 17Br 1, 30Brl 49brl R/R(O, 23) T=23”C P kbar Table 46.
Guided by the well documented sensitivity of thermopower upon sample purity and the significant improvement in sample quality during the last 25 years, we have limited the entries to work done since the mid1950’s wherever possible. This time demarcation has several additional advantages; (i) the earlier studies have been presented in an excellent summary by Nystrom [59 Ny] and thus a comparison of all work upon a given metal is readily available and (ii) this later time period includes the initial discovery and documentations of phonon-drag contributions.
39 (1978) C6-31. : Phys. Status Solidi (a) 64 (1981) K13. : Phys. Rev. B24 (1981) 4136. : Phys. Rev. B24 (1981) 1643. : J. Phys. F 11 (1981) 633. W. ” London: G. , 1949. ). G. , Turnbull, D. ), 1965. 1 Introduction [Ref. p. Therefore, only a few measurementsof Thomson heat have been done and subsequentstudies have involved the voltages AU generatedfrom thermocouples for which where A and B are the materials forming the thermocouple. Studies based upon Eq. (2) can not produce absolute thermopower results for a given material unless the absolute thermopower of one material in the thermocouple is known.
Electrical Resistivity, Thermoelectrical Power and Optical Properties by J. Bass (auth.), K.-H. Hellwege, J. L. Olsen (eds.)