SOLUTION ˜ PART I · Solute + Solvent Solution Solute + Solvent Solution Temperature y Pressure...

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SOLUTION - PART I which gets dissolves and is present in the smaller quantity Which gets dissolved and is present in the smaller quantity p1 is the vapour pressure of pure component 1 at the same temperature 0 Present in larger quantity, state of solution is determined by it Solution : Homogeneous mixture of two or more substances Types of Solution Expressing the concentration of Solutions Solubility: Maximum amount of a substance that can be dissolved in a specified amount of solvent at a specified temperature Vapour pressure of liquid solutions : Pressure formed by the vapor of the liquid over the surface of the liquid. Solute Type of Solvent Solvent Is water Aqueous Large amounts of solute in the given solvent. Concentrated Can dissolve more solute Unsaturated Lower concentration of solute Hypotonic Same concentration Isotonic Higher concentration of solute Hypertonic Cannot dissolve more solute Saturated Solute is present inexcess andcan be dissolved by increasing temperature Super saturated Small amount of solute in a large amount of solvent. Dilute Solvent Is other than water Non-Aqueous Amount of Solvent Amount of Solute Raoult’s law: “For a solution of volatile liquids, the partial vapour pressure of each component of the solution is directly proportional to its mole fraction present in solution Liquid-Liquid solutions (Components 1 and 2 both are volatile) Solid-Liquid solutions (Component 1 is volatile) Amount of solute in two solutions Solvent p1 ∞ x1 p1 = p1 x1 0 P1 ∞ x1 P1 = P1 x1 0 P1 = P1 + P2 P total = x1P1 + x2P2 = (1 - x2 )P1 + x2P2 = P1 + (P2 - P1 )x2 0 0 0 0 0 0 0 Solute Solvent Solution X 1 = 1 X 2 = 0 P T = P 1 + P 2 X 1 = 0 X 2 = 1 Mole Fraction Vapour Pressure P 1 0 P 2 = P 2 .X 2 0 P 1 = P 1 .X 1 0 P 2 0 Mole Fraction of solvent 0 1 Vapour Pressure X 1 Vapour pressure of pure solvent • Polar solutes dissolve in polar solvents and non polar solutes in non-polar solvents. • If endothermic the solubility increases with rise in temperature • Solids are incompressible hence pressure has no effect on solubility • As gases are completely compressible , their solubility increases with increase in pressure • if exothermic the solubility should decrease with rise in temperature • Many gases like oxygen are soluble in liquids like water • Dissolution of gas is predominantly exothermic hence solubility decreases with rise in temperature Solubility of a solid in a liquid Solubility of a gas in a liquid Solute + Solvent Solution Solute + Solvent Solution Temperature Solubility Pressure Solubility Solid Pressure Solubility Gas Mass percentage Volume percentage Mass by Volume percentage Parts per million(ppm) Molarity, (M) (mol L -1 ) Molality, (m) (mol kg -1 ) Mole fraction, (x) Method of Expressing Formula % = w W w2 w1 + w2 × 100 x1 = n1 n1 + n2 or x2 = n1 n1 + n2 , , y1 = P1 P1 + P2 or y2 = P1 P1 + P2 × 10 6 w2 (w1 + w2) % = v V V2 V1 + V2 × 100 % = w V w2 V solution(in ml) × 100 w2 × 1000 M2 × V solution(in ml) w2 × 1000 M2 × w1 (in g) (x1 + x2 = 1) In case of gases only, (y1 + y2 = 1)

Transcript of SOLUTION ˜ PART I · Solute + Solvent Solution Solute + Solvent Solution Temperature y Pressure...

Page 1: SOLUTION ˜ PART I · Solute + Solvent Solution Solute + Solvent Solution Temperature y Pressure ySolid Pressure Gas Mass percentage Volume percentage Mass by Volume percentage Parts

SOLUTION - PART I

which gets dissolves and is present in the smaller quantity Which gets dissolved andis present in the smaller quantity

p1 is the vapour pressure of pure component 1 at the same temperature0

Present in larger quantity, state of solutionis determined by it

Solution : Homogeneous mixture of two or more substances

Types of Solution

Expressing the concentration of Solutions

Solubility: Maximum amount of a substance that can be dissolved in a speci�ed amount of solvent at a speci�ed temperature

Vapour pressure of liquid solutions : Pressure formed by the vapor of the liquid over the surface of the liquid.

Solute

Type of Solvent

Solvent Is waterAqueous

Large amounts ofsolute in the given

solvent.

Concentrated

Can dissolve moresolute

Unsaturated

Lower concentrationof solute

HypotonicSame concentration

IsotonicHigher concentration

of solute

Hypertonic

Cannot dissolve more solute

SaturatedSolute is present inexcessandcan be dissolved byincreasing temperature

Super saturated

Small amount ofsolute in a large

amount of solvent.

Dilute Solvent Is other

than water

Non-Aqueous

Amount of Solvent

Amount of Solute

Raoult’s law: “For a solution of volatile liquids, the partial vapour pressure of each component of the solution is directly proportional to its mole fraction present in solution

Liquid-Liquid solutions(Components 1 and 2 both are volatile)

Solid-Liquid solutions(Component 1 is volatile)

Amount of solute in two solutions

Solvent

p1 ∞ x1p1 = p1 x10

P1 ∞ x1P1 = P1 x10

P1 = P1 + P2Ptotal = x1P1 + x2P2 = (1 - x2 )P1 + x2P2 = P1 + (P2 - P1 )x2

0

0

0 0 0

0

0

Solute

Solvent Solution

X1 = 1X2 = 0

PT = P1 + P2

X1 = 0X2 = 1

Mole Fraction

Vapo

ur P

ress

ure

P10

P2= P2.X20

P1= P1.X1

0

P20

Mole Fraction of solvent0 1

Vapo

ur P

ress

ure

X1

Vapour pressureof pure solvent

• Polar solutes dissolve in polar solvents and non polar solutes in non-polar solvents.

• If endothermic the solubility increases with rise in temperature

• Solids are incompressible hence pressure has no e�ect on solubility

• As gases are completely compressible , their solubility increases with increase in pressure

• if exothermic the solubility should decrease with rise in temperature

• Many gases like oxygen are soluble in liquids like water

• Dissolution of gas is predominantly exothermic hence solubility decreases with rise in temperature

Solubility of a solid in a liquid Solubility of a gas in a liquid

Solute + Solvent Solution Solute + Solvent Solution

Temperature

Solu

bilit

y

Pressure

Solu

bilit

y Solid

Pressure

Solu

bilit

y Gas

Mass percentage

Volume percentage

Mass by Volume percentage

Parts per million(ppm)

Molarity, (M)(mol L-1)

Molality, (m)(mol kg-1)

Mole fraction,(x)

Method of Expressing Formula

% =w—Ww2

w1 + w2× 100

x1 = n1n1 + n2 or x2 = n1

n1 + n2,

,y1 = P1P1 + P2

or y2 = P1P1 + P2

× 106w2(w1 + w2)

% =v—VV2

V1 + V2× 100

% =w—Vw2

Vsolution(in ml)× 100

w2 × 1000M2 × Vsolution(in ml)

w2 × 1000M2 × w1(in g)

(x1 + x2 = 1)In case of gases only,

(y1 + y2 = 1)

Page 2: SOLUTION ˜ PART I · Solute + Solvent Solution Solute + Solvent Solution Temperature y Pressure ySolid Pressure Gas Mass percentage Volume percentage Mass by Volume percentage Parts

SOLUTION - PART II

• Obey Raoult’s law over the entire range of concentration• ∆mix H = 0• ∆mix V = 0

• Do not obey Raoult’s law over the entire range of concentrationNegative deviation

Colligative Propertiesdepend on the number and not nature of solute

particles

• Solvent molecules always flow from lower concentration to higher concentration of solution• The pressure that just stops the flow of solvent is called osmotic pressure of the solution.

∆p1 = p1 - p1 0

• ∆mix H = -ve• ∆mix V = -ve

• A-B interactions are stronger than those between A-A or B-B

• A-B interactions are weaker than those between A-A or B-B

• ∆mix H = +ve• ∆mix V = +ve

Positive deviation

Solutions : On the basis of Raoult’s law.

Abnormal molar mass is the experimentally determined molar mass

• The experimentally determined molar mass is half than the true value

• Van’t Hoff introduced a factor i, known as the Van’t Hoff factor, to account for the extent of dissociation or association.

Correction Of the colligative property

• The molar mass calculated will be twice the expected value.

Association Dissociation

Ideal Non-ideal

• A-A and B-B interactions are equal to A-B interactions

XA = 1XB = 0

III

II

I

PTotal = PA + PB

XA = 0XB = 1XB

Mole Fraction

Vapo

ur P

ress

ure

PA0

PA

PB 0

PB

XA = 1XB = 0

XA = 0XB = 1

XB

XA

Mole Fraction

Vapour pressure of non-ideal solution

Idealsolution

Vapo

ur P

ress

ure

PAPB

XA = 1XB = 0

XA = 0XB = 1

XB

XA

Mole Fraction

Vapour pressure of non-ideal solution

Idealsolution

Vapo

ur P

ress

ure

PBPA

A-B interaction

BA

x2 = =∆p1p10

p1 - p1 0

p10

Relative lowering of vapour pressure of solvent

Elevation of Boiling point, ∆Tb = iKbmDepression of Freezing point, ∆Tf = iKfmOsmotic pressure of solution, Л = in2RT/V

n2—n1

= i.p1 - p1 0

p10

∆Tb = Tb - Tb0

∆Tb =Kb × 1000 × w2

M2 × w1

∆Tf = Tf - Tf0

KCl = K+ + Cl- 2CH3COOH G(CH3COOH)2

∆Tf = Tf m

∆Tf =Kf × w2× 1000

M2 × w1

Л V=w2RT

M2Л = CRT

or M2=w2RTЛ V

=p1 - p1 0

p10w2 × M1

M2 × w1

Mole Fraction of water

Pure water

Vapo

ur P

ress

ure

of w

ater

01 0.8 0.6 0.4 0.2 0

100

200

300

400

500

600

Tb

Tb0 ∆Tb

Temperature/K

Solvent

Solvent

1.013 baror 1 Atm

Solution

Solution

Boiling point of

Vapo

ur P

ress

ure

Tf Tf0

∆Tf

Temperature/K

Liquid Solvent

1.013 baror 1 Atm

Vapo

ur P

ress

ure Frozen Solvent Solution

C H3CO OH

H

.......

.......O OCH3 C

i =Normal molar mass

Abnormal molar mass

Observed colligative propertyCalculated colligative property

=

Total number of moles of particles after association/ dissociationNumber of moles of particles before association/ dissociation

i =

Pure water Solution

Osmoticpressure, Л

Pressure, Л

Glucose

Semipermeablemembrane

Relative Lowering of Vapour Pressure

Depression of Freezing Point Osmosis and Osmotic Pressure

Elevation of Boiling Point