Magnetic Rotatory Dispersion in Transparent Liquids

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\44i. 6ji/i 508. 6 589. 3 fj, i. 67180 1. 64586 1. 62806 at 20?o C. Observed by Flatow, Ann: d. Phys. < 12, 85, 1903. d=io. 38iXio 8 57272 Xi=204. X 394 nn observed ju= i . 70226 calculated JJL = i . 7043 -s forX 589. 3 MAGNETIC DISPERSION IN TRANSPARENT LIQUIDS 57 the agreement was considered sufficiently close. These numbers are given in lines 7 and 8 of Table II. The dispersion of carbon disulphide and a-monobromnapthalene has been more fully dis- cussed in a former paper. 1 The constant hi was then determined by substituting in equation (12) the values of H, /, C t, and Xj given in Table II, and the values of X, 6, and ^ for the wave-length 589 . 3 /z/i. This gave 3 . 95 X io~ 5 for hi, as shown in the last line of Table II, when all the quantities were expressed in c. G. S. And c. G. S. Electromagnetic units. The constants of (13) were now completely known, and (13) was then used to compute the values of for the range of the spectrum under investigation. The computed curve is shown by the dotted line, curve 2, of Figure 2.

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