✓ molar enthalpy ✓molar entropy of mixing change in molar Gibbs energy over pressure change V negative common logarithm of [OH-] molar heat capacity at constant volume ✓ molar Gibbs energy of mixing ✓ General solution of quadratic equation ✓reaction Gibbs energy at equilibrium ✓autoprotolysis of water ✓ work done by the system ✓ molar internal energy v standard reaction Gibbs energy ✓ van der Waals equation of state V entropy ✓ reversible, isothermal expansion work ✓ Ideal gas equation A. P = [nRT/(V-nb)] - a(n/V)² B. ASm= -R(XAlnxA + xBlnxB) C. ΔΗm = Cp,mΔΤ D. dGm = Vmdp E. AGM = RT(xAlnxA + xBlnxB) F. b2-4ac X= - b ± √ 2a G. AUm = CV,mAT H. AS = nCp,mln(Tf/Tj) PV = nRT 1. J. W = -nRT In(Vf/V₁) K. pOH = -log aOH™ L. W = -PexAV M.pKw = pOH + pH N. CV,m= Cp,m - R
✓ molar enthalpy ✓molar entropy of mixing change in molar Gibbs energy over pressure change V negative common logarithm of [OH-] molar heat capacity at constant volume ✓ molar Gibbs energy of mixing ✓ General solution of quadratic equation ✓reaction Gibbs energy at equilibrium ✓autoprotolysis of water ✓ work done by the system ✓ molar internal energy v standard reaction Gibbs energy ✓ van der Waals equation of state V entropy ✓ reversible, isothermal expansion work ✓ Ideal gas equation A. P = [nRT/(V-nb)] - a(n/V)² B. ASm= -R(XAlnxA + xBlnxB) C. ΔΗm = Cp,mΔΤ D. dGm = Vmdp E. AGM = RT(xAlnxA + xBlnxB) F. b2-4ac X= - b ± √ 2a G. AUm = CV,mAT H. AS = nCp,mln(Tf/Tj) PV = nRT 1. J. W = -nRT In(Vf/V₁) K. pOH = -log aOH™ L. W = -PexAV M.pKw = pOH + pH N. CV,m= Cp,m - R
Chemistry
10th Edition
ISBN:9781305957404
Author:Steven S. Zumdahl, Susan A. Zumdahl, Donald J. DeCoste
Publisher:Steven S. Zumdahl, Susan A. Zumdahl, Donald J. DeCoste
Chapter1: Chemical Foundations
Section: Chapter Questions
Problem 1RQ: Define and explain the differences between the following terms. a. law and theory b. theory and...
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Question
Match the terms
![T
T
✓ molar enthalpy
✓molar entropy of mixing
change in molar Gibbs energy over pressure
change
T
T
1
negative common logarithm of [OH-]
✓ molar heat capacity at constant volume
✓ molar Gibbs energy of mixing
✓
General solution of quadratic equation
reaction Gibbs energy at equilibrium
of water
✓autoprotolysis
work done by the system
molar internal energy
1
I
✓
✓
✓ standard reaction Gibbs energy
✓ van der Waals equation of state
✓ entropy
✓ reversible, isothermal expansion work
✓ Ideal gas equation
A. P = [nRT/(V-nb)] - a(n/V)²
B. ASm = -R(xAlnxA + xBlnxB)
c. AHm = Cp,mAT
D. dGm = Vmdp
E. AGM = RT(xAlnxA + xBlnxB)
F.
X=
- b ± √b² - 4ac
2a
G. AUm = CV,mAT
H. AS = nCp,mln(Tf/Ti)
PV = nRT
1.
J.
w = -nRT In(Vf/V₁)
K. pOH = -log aOH™
L. W = -PexAV
M.pKw = pOH + pH
N. CV,m = Cp,m - R](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2Fb4299bab-cfe6-4df1-82fa-bdefd18a2ba9%2F332073e0-8296-4fbd-84d4-50303b400dbc%2Fqe8nyc_processed.jpeg&w=3840&q=75)
Transcribed Image Text:T
T
✓ molar enthalpy
✓molar entropy of mixing
change in molar Gibbs energy over pressure
change
T
T
1
negative common logarithm of [OH-]
✓ molar heat capacity at constant volume
✓ molar Gibbs energy of mixing
✓
General solution of quadratic equation
reaction Gibbs energy at equilibrium
of water
✓autoprotolysis
work done by the system
molar internal energy
1
I
✓
✓
✓ standard reaction Gibbs energy
✓ van der Waals equation of state
✓ entropy
✓ reversible, isothermal expansion work
✓ Ideal gas equation
A. P = [nRT/(V-nb)] - a(n/V)²
B. ASm = -R(xAlnxA + xBlnxB)
c. AHm = Cp,mAT
D. dGm = Vmdp
E. AGM = RT(xAlnxA + xBlnxB)
F.
X=
- b ± √b² - 4ac
2a
G. AUm = CV,mAT
H. AS = nCp,mln(Tf/Ti)
PV = nRT
1.
J.
w = -nRT In(Vf/V₁)
K. pOH = -log aOH™
L. W = -PexAV
M.pKw = pOH + pH
N. CV,m = Cp,m - R
Transcribed Image Text:N. CV,m= Cp,m - R
AG = EvGm (products) - EvGm(reactants
P. ArGe = (-) RTInk
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