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1.9 47 0.052 1.44 46 0.050 3-2 57 0.06a 2.6 56 0.062 4.7 66 0.072 3 9 64 0.071 6.7 76 0.084 50 69 0.076 9.5 93 0.102 6.0 72 0.079 12.9 109 0. 120 71 75 0.083 19.0 115 0.126 9.0 77 0.085 12.2 90 0.099 20.2 115 0. 126 y ' 8 y y M 6 y y & ^ > < c .^ y y y ^ y 6 X^ ^ 4 e •5 Intensity 5 10 Fig. 3.— Width: Intensity, He, X5876.
Digitized by Google UNE STRUCTURE, III 117 The width of the line is seen to vary considerably with its inten- sity, more than doubling within the range available. The relation between width and intensity is approximately linear for low and moderate intensities. At great intensities the width is, if anything, less than this proportionality would indicate. At the intensity called 10, the capillary of the tube was just commencing to bum and show sodium lines, and possibly this might account for the falling-off from the linear relation at high intensities, but arc lines show a similar falling off. Plotting against a quadratic or logar- ithmic abscissa does not help matters.
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