. Carnegie Institution of Washington publication. iodide solution. Thickness insideof trough, cm. Sodium line. 2B/\Z = K. Glass,5=~u; 2S/X2 = Solution. LiquidAN Glass in AN Liquidv-i+K Glass inv-i+K 6 78 9 IO ii cm, . •5564•5505•5345•5333 •5469•5469•5475• 100 THE INTERFEROMETRY OF TABLE 24.—Submergence of glass convex lenses in mer-cury-potassic iodide solutions. Thickness of the troughinside, cm. Focal power, i diopter. Sodium , 5=; 2£/X2= Solution. Liq
. Carnegie Institution of Washington publication. iodide solution. Thickness insideof trough, cm. Sodium line. 2B/\Z = K. Glass,5=~u; 2S/X2 = Solution. LiquidAN Glass in AN Liquidv-i+K Glass inv-i+K 6 78 9 IO ii cm, . •5564•5505•5345•5333 •5469•5469•5475• 100 THE INTERFEROMETRY OF TABLE 24.—Submergence of glass convex lenses in mer-cury-potassic iodide solutions. Thickness of the troughinside, cm. Focal power, i diopter. Sodium , 5=; 2£/X2= Solution. LiquidAN Glass in AN Liquidn-i+K Glass inH-l+K I 2069 cm. 2 .1841 x .1742 .6746 345 .1692 • •1638•1565 xx .1432 / -1445 .6239•5921•5283 .5280 •6055•5805•5352•5396 x Focal power 2 diopter, xx Washed ellipses. / Concave lens. In both these series the trough was not fixed with adequate rigidity, sothat errors crept in from this source. Nevertheless, if the data are con-.
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