Measueement and Calculation 39 



by Beckmann's improved apparatus for this purpose,' a de- 

 scription of which will be found along with that for the 

 freezing-point determinations. 



The correction for temperature may be made, as in the 

 last case, by the application of the principle of Gay-Lussac 

 directly, or by interpolation between Pj, and Pf, the latter 

 having been determined by the previous method. 



The expression for the Gay-Lussac principle is of course 

 the same, mutatis mutandis, as that given above: 



in which Py is again the pressure in millimeters at the de- 

 sired temperature T, in the absolute scale, and Tj, is the 

 absolute boiling-point of the solution. For this calculation 

 the boiling-point of a weak aqueous solution may be con- 

 sidered the same as that of pure water. Thus Tj, = 373°, 

 the boiling-point of water, and T = 273 + t, where t is the 

 desired temperature in the Centigrade scale. Making these 

 changes in the above equation, 



_ 273 -ft 

 ^~ ' 373 • 



The method of interpolation is expressed by the follow- 

 ing equation: 



where P^ is the pressure at the desired temperature, t (Centi- 

 grade), and the other symbols are the same as above. 



3. Method by observed vapor tension: As has already 

 been stated, the vapor tension of the solvent is decreased by 

 the presence of a solute. It is found that, for dilute solu- 

 tions, this decrease in vapor tension is proportional to the 



IE. Beceuann, "Zur Praxis der Bestimmnng von Moleknlargewichten nach 

 der Siedemethode," Zeitschr.f. physik. Chem., Vol. VIII (1891), pp. 223-8. 



