. Carnegie Institution of Washington publication. 0 10 20 30 40 50 60 70 80 90 100 Percentage alcohol FIG. 43.—N/128 Nal. 140 130 120 no 100 90 •f 80 CJ -§ 70 ^60 50 40 30 20 10 0. 10 20 30 40 50 60 70 80 90 100 Percentage alcohol Fio. 44.— N/1024 Nal. with the curves for the actual conductivity, that in the latter the point of symmetry has been shifted from the 50 per cent mixture to the 80 per cent, and that the end on the alcohol side is not really at the 100 per cent alcohol, but is imaginary, since the line at the 100 per cent point must be extended to make the curve symmetrical. To be mo


. Carnegie Institution of Washington publication. 0 10 20 30 40 50 60 70 80 90 100 Percentage alcohol FIG. 43.—N/128 Nal. 140 130 120 no 100 90 •f 80 CJ -§ 70 ^60 50 40 30 20 10 0. 10 20 30 40 50 60 70 80 90 100 Percentage alcohol Fio. 44.— N/1024 Nal. with the curves for the actual conductivity, that in the latter the point of symmetry has been shifted from the 50 per cent mixture to the 80 per cent, and that the end on the alcohol side is not really at the 100 per cent alcohol, but is imaginary, since the line at the 100 per cent point must be extended to make the curve symmetrical. To be more exact, we see here shifting similar to that noted above in the case of the transition-point in the fluidity; only, this happens at every temperature instead of with rise in temperature. As the temperature rises the conductivity curves tend to become more and more nearly a linear function, that is, those for 35° have much less bend to them than those for 15°. A probable explanation. Please note that these images are extracted from scanned page images that may have been digitally enhanced for readability - coloration and appearance of these illustrations may not perfectly resemble the original Carnegie Institution of Washington. Washington, Carnegie Institution of Washington


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Keywords: ., bookauthorcarnegie, bookcentury1900, bookdecade1900, bookyear1902