The Elements of Qualitative Chemical Analysis, vol. 1, parts 1 and 2.: With Special Consideration of the Application of the Laws of Equilibrium and of the Modern Theories of Solution.Stieglitz, Julius
Science
The Elements of Qualitative Chemical Analysis, vol. 1, parts 1 and 2.: With Special Consideration of the Application of the Laws of Equilibrium and of the Modern Theories of Solution.
Stieglitz, Julius
Chemistry, Analytic -- Qualitative
[525] The values of this and similar equilibrium constants
are derived by means of Nernst's formula (see below) for the
potential difference between an element and solutions of its
ions. The derivation involves the assumption that this formula
expresses correctly the relation between the potential change and
the concentration change at all concentrations. This assumption
appears to be justified by all experimental indications thus far
observed. The constants are of importance, primarily, for the
calculations which can be made with their aid (see below), and
may, conservatively, be considered to be essentially "calculation
factors" ("Rechengrössen," according to Haber. See pp. 232–7,
Chapter XII). The constants may be expressed, as in the text,
in terms of (molar) ‹concentrations› of the ions, or in terms
of the ‹osmotic pressures› of the ions, a molar solution at 0°
producing an osmotic pressure of 22.4 atmospheres. Where osmotic
pressure and concentration are not strictly proportional (‹e.g.›
for concentrated solutions), the osmotic pressure, rather than the
concentration, is the determining factor and, when known, is used
in exact calculations. The plan, pursued in the text, is adopted
in order to express these constants in the terms used for all the
other equilibrium constants. It should be recalled (‹e.g.› p. 30)
that in calculations, in general, where pressure and concentration
are not strictly proportional, the pressure is the determining
factor. A third method of expressing the solution-tension relations
consists in giving the ‹potential differences›, which exist
‹between elements› and solutions of their ‹ions, in which the ions
have unit (molar) concentration›. These potential differences
are ‹functions› of the solution-tension constants, as will be
discussed below, and the constants, in terms of concentrations or
osmotic pressures, may be easily calculated, from the potential
differences, with the aid of this function (see below, and see the
table at the end of Chapter XV).
[526] According to Wilsmore's tabulation (‹Z. phys. Chem.›,
«36», 92 (1901)), the potential difference ε_{Cu, Cu^{2+}}
of copper against a 0.5 molar solution of cupric sulphate,
in which [Cu^{2+}] = 0.11, is +0.584 volt. Inserting these
values for [Cu^{2+}] and ε_{Cu, Cu^{2+}} in the equation
ε_{Cu, Cu^{2+}} = (0.0575 / 2) log([Cu^{2+}] / K) (see below)
and solving the equation for K, we find K = 8E−22. For
[Cu^{2+}] = 0.24, ε_{Cu, Cu^{2+}} is +0.594 volt and K = 8E−22. In
regard to the convention determining the signs used (in the present
case ε_{Cu, Cu^{2+}} is ‹positive›), see the footnote below, p.
262, and in regard to the definition of zero potential, to which
the potential differences used in this book refer, see the table
and summary at the end of Chapter XV.
[527] Nernst, ‹loc. cit.›, p. 151.
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