Solubility Equilibrium. Example 16.8 Calculating Molar Solubility from K sp Calculate the molar solubility of PbCl 2 in pure water. Begin by writing the.

Slides:



Advertisements
Similar presentations
Chapter 17 Free Energy and Thermodynamics
Advertisements

Spontaneous Processes
Chapter 17 Spontaneity, Entropy, and Free Energy The goal of this chapter is to answer a basic question: will a given reaction occur “by itself” at a particular.
Entropy, Free Energy, and Equilibrium
Entropy and Free Energy How to predict if a reaction can occur, given enough time? THERMODYNAMICS How to predict if a reaction can occur at a reasonable.
The entropy, S, of a system quantifies the degree of disorder or randomness in the system; larger the number of arrangements available to the system, larger.
Chapter 19. Overview Spontaneous Processes Entropy Second Law of Thermo. Standard Molar Entropy Gibbs Free Energy Free Energy & Temp. & Equil. Const.
Thermodynamics: Spontaneity, Entropy and Free Energy.
Chapter 18 Entropy, Free Energy and Equilibrium
Chemical Thermodynamics: Entropy, Free Energy and Equilibrium Chapter
Copyright McGraw-Hill 2009 Chapter 18 Entropy, Free Energy and Equilibrium.
Entropy and the 2nd Law of Thermodynamics
Daniel L. Reger Scott R. Goode David W. Ball Chapter 14 Chemical Equilibrium.
Chemical Thermodynamics. Spontaneous Processes First Law of Thermodynamics Energy is Conserved – ΔE = q + w Need value other than ΔE to determine if a.
Thermodynamics Chapter st Law of Thermodynamics Energy is conserved.  E = q + w.
CHM 112 Summer 2007 M. Prushan Chapter 17 Thermodynamics: Entropy, Free Energy, and Equilibrium.
Chemical Thermodynamics The chemistry that deals with the energy and entropy changes and the spontaneity of a chemical process.
CHEMICAL THERMODYNAMICS The Second Law of Thermodynamics: The is an inherent direction in which any system not at equilibrium moves Processes that are.
Chemical Thermodynamics Spontaneous Processes Reversible Processes Review First Law Second LawEntropy Temperature Dependence Gibbs Free Energy Equilibrium.
Spontaneity, Entropy, and Free Energy
Spontaneity, Entropy, & Free Energy Chapter 16. 1st Law of Thermodynamics The first law of thermodynamics is a statement of the law of conservation of.
Chapter 20 Thermodynamics and Equilibrium. Overview First Law of Thermodynamics First Law of Thermodynamics Spontaneous Processes and Entropy Spontaneous.
Ch. 19: Chemical Thermodynamics (Thermochemistry II) Chemical thermodynamics is concerned with energy relationships in chemical reactions. - We consider.
Ch. 20: Entropy and Free Energy
Chapter 19 – Principles of Reactivity: Entropy and Free Energy Objectives: 1)Describe terms: entropy and spontaneity. 2)Predict whether a process will.
In general, the more atoms in its molecules, the greater is the entropy of a substance Entropy is a function of temperature.
Chapter 17 Free Energy and Thermodynamics Lesson 1.
CHAPTER 18 Entropy, Free Energy, and Equilibrium.
Thermodynamics Chapter 19. First Law of Thermodynamics You will recall from Chapter 5 that energy cannot be created or destroyed. Therefore, the total.
A.P. Chemistry Spontaneity, Entropy, and Free Energy.
Chapter 19 Chemical Thermodynamics HW:
THERMODYNAMICS: ENTROPY, FREE ENERGY, AND EQUILIBRIUM Chapter 17.
Chapter 18: Thermodynamics Renee Y. Becker Valencia Community College.
Ch. 16: Spontaneity, Entropy, and Free Energy 16.1 Spontaneous Processes and Entropy.
Thermodynamics 3 Thermodynamics examines the heat and work as well as spontaneity of a reaction. Spontaneity is the notion of whether.
Chapter 19: Chemical Thermodynamics Spontaneous processes… …happen without outside help …are “product favored”
11 Entropy and Free Energy How to predict if a reaction can occur, given enough time? THERMODYNAMICS How to predict if a reaction can occur at a reasonable.
Chapter 17 Free Energy and Thermodynamics. Goals Entropy (S,  S) and spontaneity Free energy;  G,  G o  G, K, product- or reactant-favored Review:
First Law of Thermodynamics – Basically the law of conservation of energy energy can be neither created nor destroyed i.e., the energy of the universe.
Thermodynamics Mr. Leavings. Objectives Use the laws of thermodynamics to solve problems, identify energy flow within a system, determine the classification.
Chemical Thermodynamics Chapter 17 Chemical Thermodynamics.
Chapter 19 Spontaneity, entropy and free energy (rev. 11/09/08)
11 © 2006 Brooks/Cole - Thomson Chemistry and Chemical Reactivity 6th Edition John C. Kotz Paul M. Treichel Gabriela C. Weaver CHAPTER 19 Principles of.
Le Chatelier’s Principle
Chapter 18 – Rates of Reactions and Equilibrium Every biological and non-biological chemical reaction in nature eventually reaches a state called equilibrium.
Keeping your balance. Equilibrium Systems at equilibrium are subject to two opposite processes occurring at the same rate Establishment of equilibrium.
Chapter 16 Spontaneity, Entropy and Free Energy Spontaneity and Entropy  A reaction that will occur without outside intervention. We can’t determine.
Entropy and Free Energy (Kotz Ch 20) - Lecture #2
Entropy, Free Energy, and Equilibrium
Spontaneity, Entropy, & Free Energy Chapter 16. 1st Law of Thermodynamics The first law of thermodynamics is a statement of the law of conservation of.
CHE 116 No. 1 Chapter Nineteen Copyright © Tyna L. Meeks All Rights Reserved.
Chapter 18 Entropy, Free Energy, and Equilibrium Overview: Spontaneity and Entropy Entropy and Probability Second Law of Thermodynamics Free Energy and.
11 Entropy and Free Energy How to predict if a reaction can occur, given enough time? THERMODYNAMICS How to predict if a reaction can occur at a reasonable.
Predicting and Calculating Entropy
Chemistry 101 : Chap. 19 Chemical Thermodynamics (1) Spontaneous Processes (2) Entropy and The Second Law of Thermodynamics (3) Molecular Interpretation.
Entropy, Free Energy, and Equilibrium Chapter 18 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Chapter 19 Chemical Thermodynamics Entropy, Enthalpy, and Free Energy.
Chapter 19: Thermodynamics First Law of Thermodynamics: energy cannot be created or destroyed -total energy of the universe cannot change -you can transfer.
Chemical Thermodynamics First Law of Thermodynamics You will recall from earlier this year that energy cannot be created nor destroyed. Therefore, the.
THERMODYNAMICS – ENTROPY AND FREE ENERGY 3A-1 (of 14) Thermodynamics studies the energy of a system, how much work a system could produce, and how to predict.
Chapter 17 Free Energy and Thermodynamics 2008, Prentice Hall Chemistry: A Molecular Approach, 1 st Ed. Nivaldo Tro Roy Kennedy Massachusetts Bay Community.
Entropy and Free Energy Thermodynamics: the science of energy transfer – Objective: To learn how chemists predict when reactions will be product-favored.
Chapter 19 Spontaneity, entropy and free energy (rev. 11/09/08)
Chapter 17: Free Energy & Thermodynamics CHE 124: General Chemistry II Dr. Jerome Williams, Ph.D. Saint Leo University.
Chapter 17 Lesson 2 Free Energy and Thermodynamics.
SPONTANEOUS REACTIONS. Spontaneity 1 st Law of Thermodynamics- energy of the universe is ________. Spontaneous Rxns occur without any outside intervention.
Chapter 19 Chemical Thermodynamics
Chapter 19 Chemical Thermodynamics
Chapter 17 Free Energy and Thermodynamics
Entropy.
Presentation transcript:

Solubility Equilibrium

Example 16.8 Calculating Molar Solubility from K sp Calculate the molar solubility of PbCl 2 in pure water. Begin by writing the reaction by which solid PbCl 2 dissolves into its constituent aqueous ions and write the corresponding expression for K sp. Use the stoichiometry of the reaction to prepare an ICE table, showing the equilibrium concentrations of Pb 2+ and Cl – relative to S, the amount of PbCl 2 that dissolves. Substitute the equilibrium expressions for [Pb 2+ ] and [Cl – ] from the previous step into the expression for K sp. SOLUTION

Therefore, Example 16.8 Calculating Molar Solubility from K sp Continued Solve for S and substitute the numerical value of K sp (from Table 16.2) to calculate S. SOLUTION For Practice 16.8 Calculate the molar solubility of Fe(OH) 2 in pure water.

Example 16.9 Calculating K sp from Molar Solubility The molar solubility of Ag 2 SO 4 in pure water is –5 M. Calculate K sp. Begin by writing the reaction by which solid Ag 2 SO 4 dissolves into its constituent aqueous ions and write the corresponding expression for K sp. Use an ICE table to define [Ag + ] and [SO 4 2– ] in terms of S, the amount of Ag 2 SO 4 that dissolves. Substitute the expressions for [Ag + ] and [SO 4 2– ] from the previous step into the expression for K sp. Substitute the given value of the molar solubility for S and compute K sp. SOLUTION For Practice 16.9 The molar solubility of AgBr in pure water is –7 M. Calculate K sp.

Example Calculating Molar Solubility in the Presence of a Common Ion What is the molar solubility of CaF 2 in a solution containing M NaF? Begin by writing the reaction by which solid CaF 2 dissolves into its constituent aqueous ions and write the corresponding expression for K sp. Use the stoichiometry of the reaction to prepare an ICE table showing the initial concentration of the common ion. Fill in the equilibrium concentrations of Ca 2+ and F – relative to S, the amount of CaF 2 that dissolves. SOLUTION

Substitute the equilibrium expressions for [Ca 2+ ] and [F – ] from the previous step into the expression for K sp. Since K sp is small, we can make the approximation that 2S is much less than and will therefore be insignificant when added to (this is similar to the x is small approximation that we have made for many equilibrium problems). Solve for S and substitute the numerical value of K sp (from Table 16.2) to calculate S. Note that the calculated value of S is indeed small compared to 0.100, so our approximation is valid. Example Calculating Molar Solubility in the Presence of a Common Ion Continued SOLUTION

For comparison, the molar solubility of CaF 2 in pure water is –4 M, which means CaF 2 is over 20,000 times more soluble in water than in the NaF solution. (Confirm this for yourself by calculating the solubility in pure water from the value of K sp.) For Practice Calculate the molar solubility of CaF 2 in a solution containing M Ca(NO 3 ) 2. Example Calculating Molar Solubility in the Presence of a Common Ion Continued SOLUTION

Thermodynamics: Entropy, Gibbs Free Energy and Equilibrium

Molecular complexity – The larger the molecule, the more spatial movements. Temperature elevation/ energy flow – Hot flows to cold Reactions whose products are in more random state – S solid < S liquid < S gas Reactions that have greater number of product molecules than reactant molecules Increases in Entropy:  S > 0

Entropy and Phase Changes H 2 O(l)  H 2 O(g) Greater entropy H 2 O(s)  H 2 O(l) Lower entropy

Problem: Problem: Predict whether  S system is (+) or (−) for each of the following. Heating air in a balloon Water vapor condensing Separation of oil and vinegar salad dressing Dissolving sugar in tea 2 HgO(s)  2 Hg(l) + O 2 (g) 2 NH 3 (g)  N 2 (g) + 3 H 2 (g) Ag + (aq) + Cl − (aq)  AgCl(s)

(+)Heating air in a balloon (+) (-)Water vapor condensing (-) (-)Separation of oil and vinegar salad dressing (-) (+)Dissolving sugar in tea (+) (+)2 HgO(s)  2 Hg(l) + O 2 (g) (+) (+)2 NH 3 (g)  N 2 (g) + 3 H 2 (g) (+) (-)Ag + (aq) + Cl − (aq)  AgCl(s) (-)

PROBLEM: Determine the  S o for the chemical reaction (system): 2 H 2 (g) + O 2 (g)  2 H 2 O(l)  S system =  S reaction =  (S° prod ) −  (S° react ) ∆S o = [2 S o (H 2 O(l))] - [(2 S o (H 2 )(g)) + (S o (O 2 )(g))] ∆S o = [2 mol (69.9 J/K·mol)] - [2 mol (130.7 J/K·mol) + 1 mol (205.3 J/K·mol)] ∆S o = J/K decrease in S Note that there is a decrease in S because 3 mol of gas give 2 mol of liquid.

1 st Law: Energy (E) in the universe is conserved.  E universe =  E system +  E surroundings  E system = q + w (heat + work or P  V)  H = q (at constant P)  E =  H + P  V 2 nd Law: Total entropy (S) of the universe (total) MUST increase in a spontaneous process.  S universe =  S system +  S surroundings > 0 3 rd Law: Entropy of a substance at absolute zero (0K) for a pure substance is zero. Laws of thermodynamics

Spontaneity Criteria: Gibbs Free Energy,  G  S universe =  S system +  S surroundings > 0  S surroundings = -  H system / T  S universe =  S system -  H system / T > 0 T  S universe = T  S system -  H system > 0 -T  S universe = -T  S system +  H system < 0 -T  S universe =  G system  G =  H system - T  S system < 0

 G o Value Summary Table ∆G o = ∆H o - T∆S o Temperature INDEPENDENT ∆H o ∆S o ∆G o Reaction Spontaneity exo(–) increase(+) – Product favored Spontaneous endo(+) decrease(-) + Reactant favored Not spontaneous Temperature DEPENDENT ∆H o ∆S o ∆G o Reaction Spontaneity exo(–) decrease(-) + High temperature Not spontaneous exo(–) decrease(-) - Low temperature Spontaneous endo(+) increase(+) - High temperature Spontaneous endo(+) increase(+) + Low temperature Not spontaneous

Problem Problem: Calculate  G  at 25  C for CH 4 (g) + 8 O 2 (g)  CO 2 (g) + 2 H 2 O(g) + 4 O 3 (g). Given: Substance  G  kJ/mol CH 4 (g) − 50.5 O2(g)O2(g)0.0 CO 2 (g) − H 2 O(g) − O3(g)O3(g)163.2 Solution:  G o = (  G products o –  G reactants o )  G o = [( kJ/mol x 1 mol) + ( kJ/mol x 2 mol)] - [(-50.5 kJ/mol x 1 mol) + 0 kJ]  G o = kJ

Problem :  H = kJ,  S = J/K, T = 298 K  G =  H - T  S Problem: Calculate  G and determine whether the reaction below is spontaneous. CCl 4 (g)  C (s, graphite) + 2 Cl 2 (g) Given:  H = kJ,  S = J/K, T = 298 K  G =  H - T  S Since  G is +, the reaction is not spontaneous at this temperature. Since  G is +, the reaction is not spontaneous at this temperature. To make it spontaneous, we need to increase the temperature. To make it spontaneous, we need to increase the temperature. Solution:  G = kJ – {(298 K)( J/K)}  G = 53.5 kJ

Problem: Problem: The ∆G o for the reaction N 2 O 4  2 NO 2 is +4.8 kJ. Calculate K for this reaction. ∆G o = -RT lnK ∆G o = -RT lnK Answer Answer: ∆G o = J = - (8.31 J/K)(298 K) ln K ln K = - (4800 J/{(8.31 J/K(298 K)} ln K = Take the antilog of both sides : K = e K = 0.14 When ∆G o > 0, K < 1. When ∆G o > 0, the reaction is not spontaneous in that direction; reaction is reactant favored according to K value.