«Osmosis and Gas Pressure.»—The legitimacy of the interpretation given is most strikingly shown by experiments with a membrane, semipermeable for gases, which enables us to measure gas pressures, that may be unknown, by exactly the same process as is used to measure the unknown osmotic pressure of a solute in solution. Van 't Hoff[35] and Arrhenius[36] predicted such a result, and Ramsay[37] proved by experiment the correctness of their assumptions. A mixture of nitrogen and hydrogen may be enclosed in a palladium vessel connected with a manometer (see Fig. 6).[38] The partial pressure ‹P›_{ ‹N›} of the nitrogen may be [p025] determined by surrounding the palladium vessel with pure hydrogen, at a pressure which is known and is greater than the partial pressure of the hydrogen in the vessel, and by observing the final total gas pressure which is obtained in the vessel. The hydrogen diffuses from the point of higher concentration, outside of the vessel, through the palladium, into the interior where the concentration of the hydrogen is lower. The experiment may be carried out at 280°, a temperature at which palladium readily dissolves hydrogen and is permeable to it. The metal does not dissolve nitrogen and is not permeable to it. The volume of the enclosed gas is kept constant by raising the mercury level in the outside arm of the manometer, and the total pressure of the enclosed gas is measured when equilibrium is reached. If this total pressure is ‹P›_{ final} and the known pressure of the hydrogen outside of the vessel is ‹P›_{ ‹H›}, then, if equilibrium is reached when the hydrogen on both sides of the semipermeable palladium membrane has the same concentration (pressure), ‹P›_{ ‹H›} + ‹P›_{ ‹N›} = ‹P›_{ final} and ‹P›_{ ‹N›} = ‹P›_{ final} − ‹P›_{ ‹H›}. In other words, the excess of the final combined pressure inside, over the outside pressure of the hydrogen, ‹is equal to the pressure of the nitrogen in the vessel›. Ramsay's results showed that the amount of hydrogen actually entering the vessel was 90–97% of the amount predicted by the theory on the basis of the assumption that equilibrium will be reached, when the hydrogen has the same concentration (pressure) on both sides of the palladium membrane.