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Chapter 13 Properties of Solutions

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Chapter 13 Properties of Solutions. MQ-1 on Monday, Jan. 31 at 6:30 pm Covering Chapters 10, 11, and 13. Review session on Sunday, Jan 30 at 11:00 am – 1:00 pm in MP1000. First MQ exam – Chem 122 Monday, 31 January 6:30 pm. LAB INSTRUCTOR LOCATION - PowerPoint PPT Presentation
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Chapter 13 Properties of Solutions MQ-1 on Monday, Jan. 31 at 6:30 pm Covering Chapters 10, 11, and 13 Review session on Sunday, Jan 30 at 11:00 am – 1:00 pm in MP1000
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Page 1: Chapter 13 Properties of Solutions

Chapter 13 Properties of Solutions

MQ-1 on Monday, Jan. 31 at 6:30 pm

Covering Chapters 10, 11, and 13

Review session on Sunday, Jan 30at 11:00 am – 1:00 pm

in MP1000

Page 2: Chapter 13 Properties of Solutions

First MQ exam – Chem 122Monday, 31 January

6:30 pmLAB INSTRUCTOR LOCATION

Christopher Beekman* 250 Knowlton Hall

Chitanya Patwardhan “

Ramesh Sharma “

Mark Lobas 180 Hagerty Hall

Edwin Motari* “

Roxana Sierra “

Lin Sun “

All Others 131 Hitchcock Hall

Knowlton Hall - 2073 Neil AvenueHitchcock Hall - 2070 Neil AvenueHagerty Hall - 1775 College Rd

Page 3: Chapter 13 Properties of Solutions

Week 4 Sections 13.1- 13.6

13.1 The Solution ProcessEnergy Changes, Entropy, Rxns

13.2 Saturated Solutions and Solubility13.3 Factors Affecting Solubility

Solute-Solvent InteractionsPressure EffectsTemperature Effects

13.4 Ways of Expressing ConcentrationMass Percentage, ppm, and ppbMole Fraction, Molarity, and MolalityConversion of Concentration Units

13.5 Colligative Properties13.6 Colloids

Page 4: Chapter 13 Properties of Solutions
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Realize there is an inherent tendency for the two isolated materials to form solution,regardless of the energetics!!! This represents an entropy factor.

Page 9: Chapter 13 Properties of Solutions

Factors that FAVOR solubility:

1. Strong solute-solvent interactions

2. Weak solute-solute interactions

3. Weak solvent-solvent interactions

More often we’ll settle for the solute-solvent interactionsbeing similar to the solute-solute and solvent-solventinteractions.

A general rule: Like dissolves like.

i.e. polar and polar

non-polar and non-polar

Page 10: Chapter 13 Properties of Solutions

• Dissolution: solute + solvent solution.• Crystallization: solution solute + solvent.• Saturation: crystallization and dissolution are in

equilibrium.• Solubility: amount of solute required to form a saturated

solution.• Supersaturation: a solution formed when more solute is

dissolved than in a saturated solution.

Page 11: Chapter 13 Properties of Solutions

Fig 13.12 Structure of glucose—note red O atoms in OH groups

which can interact nicely with water.

Page 12: Chapter 13 Properties of Solutions
Page 13: Chapter 13 Properties of Solutions

Consider gas solubilities in water at 20 oC with 1 atm gas pressure (~Table 13.2)

Solubility/M

He 0.40 x 10-3

N2 0.69 x 10-3

CO 1.04 x 10-3

O2 1.38 x 10-3

Ar 1.50 x 10-3

Kr 2.79 x 10-3

CO2 3.1 x 10-2

NH3 ~ 53

Page 14: Chapter 13 Properties of Solutions

Fig 13.14 Henry’s Law, Cg = k Pg Note Table 13.2 again for k

Page 15: Chapter 13 Properties of Solutions

Consider N2 dissolved in water at 4.0 atm. Note k = 0.69 x 10-3 mol/L-atm

Cg = k Pg

= (0.69 x 10-3 mol/L-atm)(4.0 atm) = 2.76 x 10-3 mol/L

at normal atmospheric conditions, however, Pg = 0.78 atm

Cg = (0.69 x 10-3 mol/L-atm)(0.78 atm)

= 0.538 x 10-3 mol/L

Note that (2.76 - 0.54) x 10-3 mol/L = 2.22 x 10-3 mol/l

Thus for 1.0 L of water, 0.0022 mol of nitrogen wouldbe released = 0.0022 x 22.4L = 0.049 L = 49 mL !

To read about nitrogen narcosis, see http://www.scuba-doc.com/narked.html and about the bends,see http://www.diversalertnetwork.org/medical/articles/index.asp

Page 16: Chapter 13 Properties of Solutions

Solubility of GASES as a Function of Temperature

Page 17: Chapter 13 Properties of Solutions

Are these exothermic or endothermic processes?

And of

SALTS

Page 18: Chapter 13 Properties of Solutions

Ways of expressing concentration:

a) percent, ppm, ppb usually m/m

b) mole fraction = XA , XB sum of Xi = 1

c) molarity = M or mol/Lsolution

depends on T and density of solnpreparation requires dilution

d) molality = m or mol/kgsolvent

independent of Teasily prepared

Page 19: Chapter 13 Properties of Solutions

(a) Prepare 0.500 L of a 0.100 M aqueous solution of KHCO3 (MW = 100.12 g)

Recall M=n/L or n = (M)(L)therefore we need

5.01 g of KHCO3 dissolved and diluted to 0.500 L

(b) Use this solution as a ‘stock’ solution to prepare a final solution of 0.0400 M concentration.

What is the final volume of this solution?

Since n = M V, M1V1 = M2V2

and V2 = M1V1/M2 = (0.100 M)(0.500 L) / (0.0400 M)

= 1.25 L

Page 20: Chapter 13 Properties of Solutions

Consider a solution prepared by dissolving 22.4 g MgCl2 in 0.200 L of water. Assume the density of water is 1.000 g/cm3 and the density of the solution is 1.089 g/cm3.

Calculate mole fraction molarity molality

Page 21: Chapter 13 Properties of Solutions

First MQ exam – Chem 122Monday, 31 January

6:30 pmLAB INSTRUCTOR LOCATION

Christopher Beekman* 250 Knowlton Hall

Chitanya Patwardhan “

Ramesh Sharma “

Mark Lobas 180 Hagerty Hall

Edwin Motari* “

Roxana Sierra “

Lin Sun “

All Others 131 Hitchcock Hall

Knowlton Hall - 2073 Neil AvenueHitchcock Hall - 2070 Neil AvenueHagerty Hall - 1775 College Rd

Page 22: Chapter 13 Properties of Solutions

A 9.386 M solution of H2SO4 has a density of 1.509 g/cm3.

Calculatemolality% by massmole fraction of H2SO4

Page 23: Chapter 13 Properties of Solutions

Week 4 Sections 13.1- 13.6

13.3 Factors Affecting Solubility

13.4 Ways of Expressing ConcentrationMass Percentage, ppm, and ppbMole Fraction, Molarity, and MolalityConversion of Concentration Units

13.5 Colligative PropertiesLowering the Vapor PressureBoiling-Point ElevationFreezing-Point DepressionOsmosisDetermination of Molar Mass

13.6 Colloids

Page 24: Chapter 13 Properties of Solutions

Colligative Properties

Solution properties that depend only on thetotal # of ‘particles’ present.

Vapor Pressure

Boiling Point

Freezing Point

Osmotic Pressure

Page 25: Chapter 13 Properties of Solutions

Note that VP of a solution is lower than that of pure solvent.

Page 26: Chapter 13 Properties of Solutions

A fascinating and somewhat surprising observation:

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Vapor Pressure lowering

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Raoult’s Law PA = XA PAo

PA = vapor pressure over solution

XA = mole fraction of component A (solvent)

PAo = vapor pressure of pure

component A (solvent)

also PA = (1 – XB) PAo

where XB = mol fraction of B (solute)

(Recall also Dalton’s Law: PA = XA Ptotal )

Page 29: Chapter 13 Properties of Solutions

At first, we consider only nonvolatile solutes.

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Page 31: Chapter 13 Properties of Solutions

At 25 oC, the vapor pressure of benzene is 0.1252 atm,i.e. PA

o = 0.1252 atm. If 6.40 g of naphthalene (C10H8,128.17 g/mol) is dissolved in 78.0 g of benzene (78.0 g/mol),calculate the vapor pressure of benzene over the solution

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Page 35: Chapter 13 Properties of Solutions

As shown on page 503, we also can considersolutions with two volatile components.

Consider a liquid soln containing 1.0 mol benzeneand 2.0 mol of toluene at 20 oC. This yields Xbenzene = 0.33 and Xtoluene = 0.67

This can be coupled with the fact thatPo

benzene = 75 torrPo

toluene = 22 torr

Apply Raoult’s law to each separately, to obtain Pbenzene = XbenzenePo

benzene = 25 torr Ptoluene = Xtoluene Po

toluene = 15 torr and PT = Pb + Pt = 40 torr

Page 36: Chapter 13 Properties of Solutions

But with Pb = 25 torr and Pt = 15 torr

We also can calculate the concentrationsof the two in the gas phase!

Xbgas = 25/40 = 0.63

and Xtgas = 15/40 = 0.37

Page 37: Chapter 13 Properties of Solutions

Boiling Point Elevation and Freezing Point Depression(directly related to Raoult’s Law)

Page 38: Chapter 13 Properties of Solutions

Boiling Point Elevation

ΔTb = Tb final– Tb initial= Kb m => + quantity

where m is the molal concentration

Freezing Point Depression

ΔTf = Tffinal – Tf

initial = - Kf m => - quantity

where m is the molal concentration.

[note the definition and the negative sign!!!]

for H2O, Kb = 0.052 oC/m and Kf = 1.86 oC/m

Page 39: Chapter 13 Properties of Solutions
Page 40: Chapter 13 Properties of Solutions

Consider a water solution which has 0.500 molof sucrose in 1.000 kg of water. Therefore ithas a concentration of 0.500 molal or 0.500 mol/kg.

recall Kb = 0.52 oC/m and Kf = 1.86 oC/m

What is the boiling point and freezing point of this solution?

Page 41: Chapter 13 Properties of Solutions

(a) When 5.50 g of biphenyl (C12H10, 154.2 g/mol) is dissolved in 100 g benzene (C6H6, 78.0 g/mol), theBP increases by 0.903 oC. Calculate Kb for benzene.

Page 42: Chapter 13 Properties of Solutions

(a) When 5.50 g of biphenyl (C12H10, 154.2 g/mol) is dissolved in 100 g benzene (C6H6, 78.0 g/mol), theBP increases by 0.903 oC. Calculate Kb for benzene.

Kb = 2.53 K kg/mol

(b) When 6.30 g of an unknown hydrocarbon is dissolvedin 150.0 g of benzene, the BP of the solution increasesby 0.597 oC.

What is the MW of the unknown substance?

Page 43: Chapter 13 Properties of Solutions

A sample of sea water contains the following in 1.000 Lof solution. Estimate the freezing point of this solution.

Na+ = 4.58 mol Cl- = 0.533 molMg2+ = 0.052 mol SO4

2- = 0.028 molCa2+ = 0.010 mol HCO3

- = 0.002 molK+ = 0.010 Br- = 0.001 molneutral species = 0.001 mol

Sum of species = 1.095 mol

But recall we said Colligative Properties depend on thetotal concentration of ‘species’.

Page 44: Chapter 13 Properties of Solutions

Consider Exercise 13.9

List the following aqueous solutions in increasing order of their expected freezing points.

0.050 m CaCl20.15 m NaCl0.10 m HCl0.050 m HOAc0.10 m C12H22O11

Page 45: Chapter 13 Properties of Solutions

Consider Exercise 13.9

List the following aqueous solutions in increasing order of their expected freezing points.

0.050 m CaCl2 x 3 = 0.1500.15 m NaCl x 2 = 0.300.10 m HCl x 2 = 0.200.050 m HOAc x 1 = 0.0500.10 m C12H22O11 x 1 = 0.10

These calculations assume total dissociation of thesalts and zero dissociation of the last two.

The van’t Hoft “i factor”

Page 46: Chapter 13 Properties of Solutions

This effect of the dissociation of electrolytes is usuallytaken into account through the van’t Hoff i factor, which can be stated formally as

ΔTb = i Kb m

Note that i may be defined as

ΔTf(actual) Kf meffective meffective

i = -------------- = ------------- = ------------ ΔTf(ideal) Kf mideal mideal

In real systems, these i factors are NOT integers, but rather fractions whose values depend on concentration.

Page 47: Chapter 13 Properties of Solutions

Focus, for example on NaCl. Notice the limiting valueas well as the values at higher concentrations.

Page 48: Chapter 13 Properties of Solutions

But how can i be less than 2.00 for NaCl?

Through this partial

association.

Page 49: Chapter 13 Properties of Solutions

Recall this observation:

Page 50: Chapter 13 Properties of Solutions

OsmoticPressure:a fascinatingbehavior.

Yet it is theresult of avery simpletendency toequalize theconcentrationsof solutions.

With the additionof the

semipermeablemembrane—

which permits onlysolvent particles

to move from oneside to the other.

Page 51: Chapter 13 Properties of Solutions

The critical part is the membrane!!!

Page 52: Chapter 13 Properties of Solutions

Osmosis (get started)

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Page 54: Chapter 13 Properties of Solutions

A VERY practical application/consequenceof Osmotic Pressure.

Page 55: Chapter 13 Properties of Solutions

Hypertonic soln

crenation (shrivels)

Hypotonic soln

hemolysis (bursts)

Page 56: Chapter 13 Properties of Solutions

Examples:– Cucumber placed in NaCl solution loses water to

shrivel up and become a pickle.– Limp carrot placed in water becomes firm because

water enters via osmosis.– Salty food causes retention of water and swelling of

tissues (edema).– Water moves into plants through osmosis.– Salt added to meat or sugar to fruit prevents bacterial

infection (a bacterium placed on the salt or honey will lose water through osmosis and die).

Page 57: Chapter 13 Properties of Solutions

Osmotic Pressure: π V = n R T

or π = (n/V) R T or π = M R T

(or π = ρ g h,

where ρ = density of solution g = 9.807 m s-2

h = height of columnbut be careful of the units with this form.)

Page 58: Chapter 13 Properties of Solutions

π = ρ g h, where ρ = density of solution g = 9.807 m s-2

h = height of column

If h = 0.17 meters of a dilute aqueous soln with ρ = 1.00 g/cm3

π = [(1.00g/cm3)(10-3 kg/g)(106 cm3/m3)](9.807 m/s2)(0.17 m)

= 1.7 x 103 kg m-1 s-1 = 1.7 x 103 Pa

or = (1.7 x 103 Pa) / (1.013 x 105 Pa / atm) = 0.016 atm

Page 59: Chapter 13 Properties of Solutions

A chemist dissolves 2.00 g of protein in 0.100 L of

water. The observed osmotic pressure is 0.021 atm at 25 oC. What is the MW of the protein?

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ColloidsColloids

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Hydrophilic and Hydrophobic Colloids• Focus on colloids in water.• “Water loving” colloids: hydrophilic.• “Water hating” colloids: hydrophobic.• Molecules arrange themselves so that hydrophobic

portions are oriented towards each other.• If a large hydrophobic macromolecule (giant molecule)

needs to exist in water (e.g. in a cell), hydrophobic molecules embed themselves into the macromolecule leaving the hydrophilic ends to interact with water.

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Page 70: Chapter 13 Properties of Solutions

Hydrophilic and Hydrophobic Colloids• Typical hydrophilic groups are polar (containing C-O, O-

H, N-H bonds) or charged.• Hydrophobic colloids need to be stabilized in water.• Adsorption: when something sticks to a surface we say

that it is adsorbed.• If ions are adsorbed onto the surface of a colloid, the

colloids appears hydrophilic and is stabilized in water.• Consider a small drop of oil in water.• Add to the water sodium stearate.

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Hydrophilic and Hydrophobic Colloids

ColloidsColloids

Page 72: Chapter 13 Properties of Solutions

Hydrophilic and Hydrophobic Colloids• Sodium stearate has a long hydrophobic tail

(CH3(CH2)16-) and a small hydrophobic head (-CO2-Na+).

• The hydrophobic tail can be absorbed into the oil drop, leaving the hydrophilic head on the surface.

• The hydrophilic heads then interact with the water and the oil drop is stabilized in water.

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Page 74: Chapter 13 Properties of Solutions

Removal of Colloidal Particles. . . . . . .

• Colloid particles are too small to be separated by physical means (e.g. filtration).

• Colloid particles are coagulated (enlarged) until they can be removed by filtration.

• Methods of coagulation:– heating (colloid particles move and are attracted to each

other when they collide);

– adding an electrolyte (neutralize the surface charges on the colloid particles).

– Dialysis: using a semipermeable membranes separate ions from colloidal particles


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