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15 K) at pressures from 9 atm to 292 atm. A comparison of these results with values predicted by the equation shows that, in ninety-nine c a s e s , the deviation is less than 0 . 18%. T h e s e small deviations are all positive and systematic, increasing along each isotherm with increasing density. ( 6 3) There is a considerable overlap b e t w e e n this work and that of Wiebe et α/. 15 K) at pressures from 100 atm to 1000 atm. T h e deviation of these results from those predicted by the equation of state lies within ± 0 .
Figure 6. 1 DENSITY Experimental m e a s u r e m e n t s of density extend from approximately 2 Κ to 500 Κ and were made by a large number of authors using a wide variety of t e c h n i q u e s : it is possible to deal with them only briefly in this section. Figure 7 shows the e x t e n t of the region covered by each group of w o r k e r s . 15 K) at pressures from 9 atm to 292 atm. A comparison of these results with values predicted by the equation shows that, in ninety-nine c a s e s , the deviation is less than 0 .
Other m e a s u r e m e n t s of the dielectric c o n s t a n t of helium at isolated t e m p e r a t u r e s , and not necessarily in the saturation state, h a v e been EXPERIMENTAL ( 5 6) RESULTS 17 ( 5 7) made by G r e b e n k e m p e r and H a g e n and Chase et α/. 122 8. K e r r and ( 5 8) Sherman, w h o have m e a s u r e d the dielectric c o n s t a n t and t h e density simultaneously over a range of t e m p e r a t u r e s and p r e s s u r e s , suggest that for helium-3 the molar polarizability is a slowly varying function of density and that the same m a y apply to helium-4.