1. At a given pressure and temperature, the phase with the highest chemical potential will be the most stable. 2. At equilibrium, the chemical potential of a substance is the same in and throughout every phase present in the system. 3. If a solute follows Henry's Law, its activity coefficient must be 0.

Chemistry: Principles and Practice
3rd Edition
ISBN:9780534420123
Author:Daniel L. Reger, Scott R. Goode, David W. Ball, Edward Mercer
Publisher:Daniel L. Reger, Scott R. Goode, David W. Ball, Edward Mercer
Chapter18: Electrochemistry
Section: Chapter Questions
Problem 18.103QE
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Answer true or false, if false then explain why
1. At a given pressure and temperature, the phase with the highest chemical potential will be
the most stable.
2. At equilibrium, the chemical potential of a substance is the same in and throughout every
phase present in the system.
3. If a solute follows Henry's Law, its activity coefficient must be 0.
4. The equilibrium constant, K, can be calculated from the measured standard cell potential
RT
In K.
vF
of an electrochemical cell according to the relationship: E
5. Degeneracies do not need to be accounted for when calculating the Boltzmann ratio
Ni/N; (i.e., the relative population of two states i and j).
6. The molecular partition function indicates the number of thermally accessible states at a
given temperature.
Transcribed Image Text:1. At a given pressure and temperature, the phase with the highest chemical potential will be the most stable. 2. At equilibrium, the chemical potential of a substance is the same in and throughout every phase present in the system. 3. If a solute follows Henry's Law, its activity coefficient must be 0. 4. The equilibrium constant, K, can be calculated from the measured standard cell potential RT In K. vF of an electrochemical cell according to the relationship: E 5. Degeneracies do not need to be accounted for when calculating the Boltzmann ratio Ni/N; (i.e., the relative population of two states i and j). 6. The molecular partition function indicates the number of thermally accessible states at a given temperature.
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