The Principles of Chemistry, Volume IMendeleyev, Dmitry Ivanovich
Science
The Principles of Chemistry, Volume I
Mendeleyev, Dmitry Ivanovich
Argon; Chemistry; Periodic law
[47] If the substance dissolved is non-volatile (like salt or sugar),
or only slightly volatile, then the whole of the tension of
the vapour given off is due to the water, but if a solution
of a volatile substance--for instance, a gas or a volatile
liquid--evaporates, then only a portion of the pressure belongs
to the water, and the whole pressure observed consists of the sum
of the pressures of the vapours of the water and of the substance
dissolved. The majority of researches bear on the first case,
which will be spoken of presently, and the observations of D. P.
Konovaloff (1881) refer to the second case. He showed that in the
case of two volatile liquids, mutually soluble in each other,
forming two layers of saturated solutions (for example, ether
and water, Note 20, p. 67), both solutions have an equal vapour
tension (in the case in point the tension of both is equal to 431
mm. of mercury at 19·8°). Further, he found that for solutions
which are formed in all proportions, the tension is either
greater (solutions of alcohol and water) or less (solutions of
formic acid) than that which answers to the rectilinear change
(proportional to the composition) from the tension of water
to the tension of the substance dissolved; thus, the tension,
for example, of a 70 p.c. solution of formic acid is less, at
all temperatures, than the tension of water and of formic acid
itself. In this case the tension of a solution is never equal to
the sum of the tensions of the dissolving liquids, as Regnault
already showed when he distinguished this case from that in
which a mixture of liquids, which are insoluble in each other,
evaporates. From this it is evident that a mutual action occurs
in solution, which diminishes the vapour tensions proper to the
individual substances, as would be expected on the supposition of
the formation of compounds in solutions, because the elasticity
then always diminishes.
[48] This amount is usually expressed by the weight of the substance
dissolved per 100 parts by weight of water. Probably it would
be better to express it by the quantity of the substance in a
definite volume of the solution--for instance, in a litre--or
by the ratios of the number of molecules of water and of the
substance dissolved.
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