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Elementary treatise on physics, experimental and applied : for the use of colleges and schools (1906)

Ganot, A. (Adolphe), 1804-1887, Atkinson, Edmund, 1831-1901, Reinold, A. W. (Arnold William), 1843-1921 · New York : Wood · leaf 117

An illustration from Elementary treatise on physics, experimental and applied : for the use of colleges and schools, 1906, leaf 117
er liquid for part of it to remain in both legsof the tube. The preceding principle may be deduced by a very simple calculation.Let <^/and d be the densities of water and mercury, and // and // their re-spective heights, and let ^ be the acceleration due to gravity. The pressureon B will be… … 100 On Liquids [106- dhg must be equal to dhg^ or dh = dh. This is nothing more than analgebraical expression of the above principle ; for since the two productsmust always be equal, d must be as many times greater than da.s Ji is lessthan //. In this manner the density of a liquid may be…

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