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Chem 300 - Ch 25/#2 Today’s To Do List Binary Solid-Liquid Phase Diagrams Continued (not in text…) Colligative Properties
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Chem 300 - Ch 25/#2 Today’s To Do List Binary Solid-Liquid Phase Diagrams Continued (not in text…) Colligative Properties.

Dec 14, 2015

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Page 1: Chem 300 - Ch 25/#2 Today’s To Do List Binary Solid-Liquid Phase Diagrams Continued (not in text…) Colligative Properties.

Chem 300 - Ch 25/#2 Today’s To Do List

• Binary Solid-Liquid Phase Diagrams Continued (not in text…)

• Colligative Properties

Page 2: Chem 300 - Ch 25/#2 Today’s To Do List Binary Solid-Liquid Phase Diagrams Continued (not in text…) Colligative Properties.

Stable Compound Formation

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K/Na with incongruent MP & Unstable Compound Formation

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Colligative Properties

Depends upon only the number of (nonvolatile) solute particles

Independent of solute identity From colligatus: “depending upon the

collection”• Vapor pressure lowering• Boiling point elevation• Freezing point depression• Osmotic pressure

Page 11: Chem 300 - Ch 25/#2 Today’s To Do List Binary Solid-Liquid Phase Diagrams Continued (not in text…) Colligative Properties.

Basis for Colligativity

Solvent chem potential (μ1) is reduced when solute is added:• μ*

1 μ*1 + RT ln x1 (“1” is solvent)

• Since x1 < 1 ln x1 < 0

• Thus μ1 (solution) < μ1 (pure solvent)

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Chemical Potential

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Vapor Pressure lowering

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Freezing Point Depression: ΔTfus = Kf m

Thermo Condition:• At fp: solid solvent in equilib with solvent

that’s in soln

• μsolid1(Tfus) = μsoln

1(Tfus)

• μsolid 1 = μ*

1 + RT ln a1 = μliq1 + RT ln a1

Rearranging:• ln a1 = (μsolid

1 - μliq1)/RT

Page 15: Chem 300 - Ch 25/#2 Today’s To Do List Binary Solid-Liquid Phase Diagrams Continued (not in text…) Colligative Properties.

ln a1 = (μsolid 1 - μliq

1)/RT

Take derivative:• ( ln a1/ T)P, x1 = [(μsolid

1 - μliq1)/RT]/ T

• Recall Gibbs-Helmholtz equation:• [ (μ/T)/ T]P, x1 = - H1/T2

• Substitute in above:

• ( ln a1/ T)P, x1 = (Hliq1 – Hsol

1)/RT2 = ΔfusH/RT2

Page 16: Chem 300 - Ch 25/#2 Today’s To Do List Binary Solid-Liquid Phase Diagrams Continued (not in text…) Colligative Properties.

( ln a1/ T)P, x1 = ΔfusH/RT2

Integrate between T*fus and Tfus :

• ln a1 = ƒ(ΔfusH/RT2)d T

Since it’s a dilute solution:• a1 ~ x1 = 1- x2

• ln (1 – x2) ~ - x2

Substitute above:• - x2 = (ΔfusH/R)(1/T*

fus – 1/Tfus)

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- x2 = (ΔfusH/R)(Tfus - T*fus)/T*

fus Tfus

Solute lowers the freezing point:• Tfus < T*

fus

Express in molality:• x2 = n2/(n1 + n2) = m/(1000/M1 + m)

• But m << 1000/M1

• x2 ~ M1m/1000 (substitute above for x2)

Note: T*fus ~ Tfus

• (Tfus - T*fus)/T*

fus Tfus ~ (Tfus - T*fus)/T*2

fus

= - Δ T/T*2fus

Page 18: Chem 300 - Ch 25/#2 Today’s To Do List Binary Solid-Liquid Phase Diagrams Continued (not in text…) Colligative Properties.

Substitute!

Δ Tfus = Kf m

• Where Kf = M1 R(T*fus)2 /(1000ΔfusH)

• Kf is function of solvent only

Similar expression obtained for bp elevation: Δ Tvap = Kb m

• Where Kb = M1 R(T*vap)2 /(1000ΔvapH)

Compare terms

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Example Comparison

Calc. fp and bp change of 25.0 mass % soln of ethylene glycol (M1 = 62.1) in H2O.

m = nGly/kg H2O = (250/62.1)/(750/103) = 5.37

Δ Tfus = Kf m = (1.86)(5.37) = 10.0 OC

Δ Tvap = Kb m = (0.52)(5.37) = 2.8 OC

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Osmotic Pressure

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Example

Calc. Osmotic pressure of previous example at 298 K.

Π = c2RT

• c2 = 4.0 R = 0.0821 L-atm/mol-K

• Π = c2RT = (4.0)(0.0821)(298) = 97 atm

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Debye-Hückel Model of Electrolyte Solutions

The Model: An electrically charged ion (q) immersed in a solvent of dielectric constant ε

Experimental Observations:• All salt (electrolyte) solutions are nonideal

even at low concentrations• Equilibrium of any ionic solute is affected by

conc. of all ions present.

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Next Time

How to explain the experimental evidence:Debye-Huckel Model of electrolyte solutions