SlideShare a Scribd company logo
Solution Colligative Properties
Presentedby:FreyaCardozo
1
Presented by:
Freya
Cardozo
Solution
 It is a homogenous mixture of two or more pure substances
 Solution= Solute + Solvent
 Solvent is the one present in larger quantity
 Solute is the one present in smaller quantities
 Solutions with only one solute are called Binary solutions
Presented by: Freya Cardozo
2
Types of solutions
 The solute and solvent can be in any of the following state solids, liquids
or gases
 Combinations of these gives mainly 9 types of solutions
Presented by: Freya Cardozo
3
Presented by: Freya Cardozo
4
Solubility
 The solubility of a solute is its amount per unit volume of
saturated solution at a specific temperature
 Solubility unit= mol L-1
Presented by: Freya Cardozo
5
Factors affecting solubility
 Nature of solute and solvent
 Effect of temperature on solubility
 Effect of pressure on solubility
Presented by: Freya Cardozo
6
Nature of solute and solvent
 Like dissolves like
 Similar chemical character are more readily soluble in each other than
different chemical natures
 Similar substances also have similar intermolecular forces of attraction
 Polar solutes dissolve in polar solvents because , solute-solute, Solute-
solvent and solvent-solvent interactions are of similar magnitude
 Eg. NaCl in water, Cholesterol in Benzene, Sugar in water
Presented by: Freya Cardozo
7
Effect of temperature on solubility
 For endothermic processes – Eg. KCl in water
↑T ↑Solubility because there is an increase in stress on the solution
 For exothermic process – CaCl2 in water
↑T ↓Solubility
But there hasn’t been any direct relation between exo and
endothermicity on T
Presented by: Freya Cardozo
8
T Vs Solubility
 NaBr, NaCl, KCl : S slightly changes with T
 KNO3, NaNO3, KBr: ↑T ↑Solubility
 Na2SO4 ↑T ↓Solubility
Gas molecules are condensed in liquid phase, this
process is exothermic. Thus, Solubility of gases in
water should decreases with increase in
temperature.
Presented by: Freya Cardozo
9
REAL LIFE EXAMPLE
Industries take billions of gallons of water from rivers and lakes to cool
down the equipment's which get heated during the industrial
production process. Once the cool water is used the hot water
produced is the returned to the water bodies again. Due to the
increase in the temperature of water the solubility of gas in water
decrease and thus it is very less available for fishes
Presented by: Freya Cardozo
10
Effect of pressure on solubility
 Pressure has no effect on solubility of liquids and solids as they are
incompressible
 But for gases the solubility is greatly influenced by pressure
 The relation between P and S for gases can be given by HENRY’S
LAW
Presented by: Freya Cardozo
11
HENRY’S LAW
 The law states that the solubility of a gas in a liquid is directly proportional to the
pressure of the gas over the solution

 Where, S= Solubilty of gase in molL-1
P=Pressure of gas over solution in bar
KH= Henry constant. Unit is mol L-1 bar-1
 When, P=1, KH=S. Thus, KH is the solubility of the gas in a liquid when its pressure over
solution is 1 bae
Presented by: Freya Cardozo
12
Example and Exceptions
 CO2 added in cold drinks under a pressure
 As compared to normal conditions under pressure the solubility is much higher
 Release relives this pressure giving the effervescence
 Exceptions are NH3 and CO2 because they react with water
 As they form these compounds they have higher solubilities than expected by
Henrys law
Presented by: Freya Cardozo
13
Type 1 numericals
 Based on Henry’s law
 S=KHP
Presented by: Freya Cardozo
14
QUESTION
 The henry’s law constant of CH3Br is 0.159 mol L-1 bar-1 at 250C.
What is the solubility of CH3Br in water at 250C and at 130mm Hg?
(1mmHg= 0.00133 bar)
Presented by: Freya Cardozo
15
RAOULT’S LAW
 The law states that, “ The partial vapour pressure of any volatile
component of a solution is equal to the vapour pressure of the
pure component multiplied by its mole fraction in the solution.”
 P= x P0
 P= partial pressure
 p0= partial pressure of pure component
 x= mole fraction
Presented by: Freya Cardozo
16
Mole fraction
 Mole fraction represents the number of molecules of a particular component in
a mixture divided by the total number of moles in the given mixture. It's a way
of expressing the concentration of a solution
 Represented by x
 The mole fraction of solute is x2 and solvent is x1; x1+x2=1
Presented by: Freya Cardozo
17
Derive Raoult’s law
1. Let A1 and A2 be two volatile liquids, P1 and P2 be the respective partial pressures
and P1
0 , P2
0 be vapour pressures of pure liquids
2. Let x1 and x2 be the mole fractions of A1 and A2 respectively
3. Raoult’s law can be written as P1= x1 P1
0 and P2 = x2 P2
0
Presented by: Freya Cardozo
18
Since, P1
0 and P2
0 are constant
P Vs x2 is a straight line
P1 Vs X1 and P2 Vs x2 are also straight line passing
through the origin
Presented by: Freya Cardozo
19
IDEAL SOLTIONS NONIDEAL
SOLUTIONS
1. Obey Raoult’s law over entire range of
concentrations
2. V.P always lies between V.P of pure components
3. No heat is evolved/ absorbed when 2
components are mixed. Enthalpy of mixing is
zero. ∆mix H=0
4. No volume change. Thus Vol of sol. Is equal to
sums of volumes of the 2 components mixed.
∆mixV=0
5. Solvent-solute, solute-solute and solvent-solvent
molecular interactions are comparable
1. Do not obey Raoult’s law over entire range
of concentrations
2. V.P of these solutions can be higher or lower
than those of pure components
3. It shows two types of deviation:
 Positive deviation
 Negative deviation
Presented by: Freya Cardozo
20
POSITIVE DEVIATION NEGATIVE DEVIATION
 Solute-solvent I.F.A (weaker)< solute-solute
I.F.A & solvent-solvent I.F.A
 V.P is higher than the pure components
 Eg. Acetone+ Ethanol
Acetone+ carbon disulphide
 Solute-solvent I.F.A (stronger)> solute-solute I.F.A
& solvent-solvent I.F.A
 V.P is higher than the pure components
 Eg. Acetone + chloroform
Phenol + Aniline
Presented by: Freya Cardozo
21
I.F.A= Intermolecular forces of attraction
Colligative properties
 Definition of colligative properties
The physical properties of solutions that depend on the number of solute particles in
solutions and not on their nature are called colligative properties
 There are 4 colligative properties
1. Vapour pressure lowering
2. Boiling point elevation
3. Freezing point depression
4. osmotic pressure
 Non-electrolytic and dilute solutions are used
Presented by: Freya Cardozo
22
Vapor pressure
 The pressure exerted by the liquid vapor over the surface of a liquid in a closed
container when both are in equilibrium is called as vapor pressure
Presented by: Freya Cardozo
23
VOLATILE SUBSTANCE NON-VOLATILE SUBSTANCE
Presented by: Freya Cardozo
24
Vapour pressure lowering
 When a non volatile non-ionizable solid is dissolved in a liquid solvent, the vapour pressure of the
solution is lower than that of the solvent.
 If the solute is non-volatile it does not contribute to the VP above the solution
 Thus VP of solution=VP of solvent above the solution
 Mathematically, If P1
0 is the VP of pure solvent and P1 is the VP of solvent above the solution, P1<
P1
0
 Thus, vapour pressure lowering is ∆= P1
0 – P1
Presented by: Freya Cardozo
25
Reason for this?
 The vapour pressure of a liquid depends on the ease
with which the molecules escape from the surface of
liquid
 When non-volatile solute is added it replaces some of
the volatile solvent molecules at the surface and these
non volatile solutes do not vaporizes and thus do not
contribute to the vapour pressure.
 Therefore, the number of solvent molecules available for
vaporization per unit surface area is less than number at
surface of pure solvent
Presented by: Freya Cardozo
26
Raoult’s law for solution of non volatile solutes OR Prove that
∆P= P1
0 x2 OR Prove lowering of vapour pressure is a
colligative property
 For a solution containing non volatile solute, the vapour pressure of
solvent over the solution is equal to the vapour pressure multiplied by its
mole fraction in the solution
P1= P1
0 x1
 For a binary solution containing 1 solute, x1=1-x2 (Since, x1+x2=1)
 But, we know that lowering of vapour pressure is given by ∆= P1
0 – P1
 Thus, ∆P= P1
0x2
 From the above equation it is clear that the ∆P depends on x2 which is
number of solute particles, thus lowering of vapour pressure is a colligative
property
Presented by: Freya Cardozo
27
Relative Lowering of Vapour pressure
 The ratio of vapour pressure lowering of solvent divided by the vapour pressure of pure solvent is
called relative lowering of vapour pressure.
 Thus,
 Relative lowering of VP is equal to the mole fraction of solute in the solution. Therefore, relative
lowering of VP is also a colligative property
Presented by: Freya Cardozo
28
Relationship between molar mass of
solute and lowering of vapour pressure
 We know that relative lowering of vapour pressure is equal to mole fraction of solute i.e.
 The mole fraction of a component of solution is equal to its moles divided by the total moles
in the solution. Thus,
 n1= moles of solvent and n2= moles of solute
 In dilute solutions, n1>>n2, thus n1+n2~n1.
 Thus the mole fraction is
Presented by: Freya Cardozo
29
 Suppose a solution is prepared by adding W2 g of solute in W1 g of solvent. The moles of
solute and solvent in the solution are,
 Where, M1 and M2 are molar masses of solvent and solute respectively. Substituting in the
equation,
Presented by: Freya Cardozo
30
WHAT DO YOU THINK?
Presented by: Freya Cardozo
31
TYPE 2 numericals
∆P= P1
0X2
Presented by: Freya Cardozo
32
Presented by: Freya Cardozo
33In an experiment, 18.04 g of mannitol was dissolved in 100 g of water. The vapour pressure of
water was lowered by 0.309 mm Hg from 17.535 mmHg. Calculate the molar mass of
mannitol
Presented by: Freya Cardozo
34
A solution is prepared by dissolving 394g of a non volatile solute is 622g of water. The vapour
pressure of solution is found be 30.74 mm Hg at 300C. If the vapour pressure at 300C is 31.8
mm Hg, what is the molar mass of solute?
Presented by: Freya Cardozo
35The vapour pressure of pure benzene (molar mass 78 g/mol) at a certain temperature is 640
mmHg. A non-volatile solute of mass 2.315g is added to 49g of benzene. Th vapour pressure
of solution is 600 mmHg. What is the molar mass of the solute?
Presented by: Freya Cardozo
36
Boiling point elevation
 B.P : The temperature at which the vapour pressure equals to the applied
pressure/ atmospheric pressure(if open container)
 Solutions with non volatile solute have higher B.P than pure solvent
 If Tb
0 is B.P of pure solvent and Tb is of the solution then the difference between
them ∆Tb
 The difference between the B.P of solution and that of the pure solvent at
any given point is called the boiling point elevation
Presented by: Freya Cardozo
37
Lowering of V.P and Elevation in B.P
1. In the graph Vapour pressure of the solvent and solution are
plotted as a function of temperature
2. From the previous discussions we know that the vapour pressure of
solution with non volatile solute<vapour pressure of pure solvent
3. Thus from graph we can see that
CD= vapour pressure of solution(lower curve)
AB= vapour pressure of pure solvent(higher curve)
4. The V.P difference goes on increasing with temperature
Presented by: Freya Cardozo
38
5. The intersection of the curves AB and CD on the X axis shows that
the boiling point of solution is more than the pure solvent
6. A liquid boils when its V.P is equal to 1 atm(atmospheric
pressure). Therefore, in order for the solution to boil a higher
temperature will be needed to reach 1 tm than the solvent.
7. That’s why the solution needs to be heated more to be boiled.
Hence, there will be elevation in the B.P of solution even though
there is a lowering of vapour pressure.
[V.P is inversely related to B.P]
Presented by: Freya Cardozo
39
Expressing concentration
MOLARITY MOLALITY
Presented by: Freya Cardozo
40
B.P elevation and conc. Of solute
1. The B.P elevation is directly proportional to molality of the solution.
2. Where, m= molality of solution
Kb= boiling point elevation constant/ molal elevation constant/ ebullioscopic constant
3. If, m=1, ∆Tb=Kb
Thus, ebullioscopic constant is the B.P elevation produced by 1 molal solution
Presented by: Freya Cardozo
41
Batao..
Presented by: Freya Cardozo
42
Why molality over molarity?
Because, we are studying systems where temperature is not constant thus we have to
choose terms that do not depend on temperature
molality is temperature independent whereas molarity depends on temperature
This can be seen from the units also
Presented by: Freya Cardozo
43
Molality= mol/kg
Molarity= mol/L
Relationship between mass of solute and
boiling point elevation
 Suppose a solution is made by dissolving W2 g of solute in W1 g of solvent
 Moles of solute in solvent= W2/ M2 (M2= molar mass)
Mass of solvent= W1g = W1 g/ 1000 g/kg = W1/ 1000 kg
 Molality can be given by
Presented by: Freya Cardozo
44
TYPE 3:
Elevation of B.P
Presented by: Freya Cardozo
45
Presented by: Freya Cardozo
46
Presented by: Freya Cardozo
47
Presented by: Freya Cardozo
48
Presented by: Freya Cardozo
49
A solution containing 0.73 g of camphor (molar mass 152 gmol-1) in 36.8 g of acetone
(boiling point 56.30C) boils at 56.55 0C. A solution of 0.564 g of unknown compound in the
same weight of acetone boils at 56.46 0C. Calculate the molar mass of the unknown
compound. [Oct 2014]
Freezing point
 Freezing of point of a liquid is the temperature at which the liquid and solid are
in equilibrium and the two phases have the same vapour pressure
Presented by: Freya Cardozo
50
Depression in Freezing point
 It is observed that addition of non volatile solute to solvent lowers the freezing
point
 Thus, The F.P of solution( with non-volatile solute)< F.P of pure solvent
 Now, if Tf
0 is freezing point of pure solvent and Tf of the solution, Tf
0 > Tf
 The difference between the two is called ∆ Tf
Presented by: Freya Cardozo
51
Freezing point depression & Vapour
pressure lowering
 Consider the vapour pressure diagram
1. Curve AB= V.P of solid solvent
2. Curve CD= V.P of pure liquid
3. Curve EF = V.P of solution
 The vapour pressure of solution is always lower than the
solvent and thus is present at the lower part of the graph
 The non-volatile solute does not dissolve in the solid solvent
Presented by: Freya Cardozo
52
 Curve AB and CD  Intersect at B – This is where both the
solid and liquid phases have the same V.P.
Thus, The temperature corresponding to point B is freezing
point of the pure solvent Tf
0
 Curve EF and AB  Intersect at E – This is the point at
which the solid solvent is in equilibrium with the solution
Thus, The temperature corresponding to point E is freezing
point of the solution Tf
 It is clear from the figure that the freezing point of solution
is lower than that of the pure solvent
Presented by: Freya Cardozo
53
But why so?
DUE TO THE ATTRACTIVE FORCES BETWEEN THE MOLECULES
 In pure liquid the attractive forces among molecules are large enough to cause
the change of phase from liquid to solid
 In solution, there are solute molecules in between the solvent particles.. this
causes more separation of solvent molecules than in the solvent
 Therefore, there is a decrease in the attractive forces between the solvent
molecules. So the temperature of the solution is lowered below the freezing point
of solvent to cause phase channge
Presented by: Freya Cardozo
54
Presented by: Freya Cardozo
55
Only solvent molecules Solute + solvent molecules
Easier to change
phase
Solute molecules obstruct the
phase change. More T
needed(Lower Temps)
Real life application
Presented by: Freya Cardozo
56
Freezing point depression and molality
 Freezing point depression ∆Tf is directly proportional to molality of the solution
 Kf= Freezing point depression constant / cryoscopic constant
 If, m=1 ; ∆Tf = Kf
 The cryoscopic constant thus is the depression in freezing point produced by 1 molal solution
of a non volatile solute
Presented by: Freya Cardozo
57
Presented by: Freya Cardozo
58
Relationship between Molar mass of
solute and F.P depression
Presented by: Freya Cardozo
59
Presented by: Freya Cardozo
60
Presented by: Freya Cardozo
61
Osmosis
 The net flow of solvent molecules into the solution through a semipermeable membrane
OR
 The net flow of solvent molecules into the solution from a more dilute solution to more
concentrated solution through a semipermeable membrane is called osmosis
Presented by: Freya Cardozo
62
SOLVENT SOLUTION Lower Conc.
Higher
conc.
Semipermeable membrane
 It is a film such as cellophane which has pores large
enough to allow the solvent molecules to pass through
them
 The pores are small enough to not allow the flow of the
larger solute molecules or ions of higher mass
 Selectively allows passage of solvent molecules
Presented by: Freya Cardozo
63
Solute
molecules
Semi-
P.M
Solvent
molecules
Osmotic pressure
 In the thistle tube solution of interest (sugar solution)
is placed and it is immersed in beaker filled with pure
water
 A semipermeable membrane is placed at the mouth
of the tube
 Some solvent passes through the membrane into the
solution
 This causes rise in liquid level in the tube
 Now, the hydrostatic pressure in the tube pushes the
solvent back into the container
Presented by: Freya Cardozo
64
Reverse osmosis
 The liquid rises in tube and then stops, when the liquid stops
rising that is the pressure which stops the flow and is called
the osmotic pressure
 This hydrostatic pressure that stops the osmosis is of the
solution is the osmotic pressureΠ and is equal to
1. Height of the liquid column
2. Density of liquid column
3. acceleration due to gravity
Presented by: Freya Cardozo
65
Presented by: Freya Cardozo
66
Type Definition Examples
Isotonic solutions Two or more solutions having the
same osmotic pressure are said to
be isotonic
No net flow of solvent in either
direction
0.1 M urea= 0.1 M sucrose
Both have equal osmotic pressure
but
Different conc in g/L
Hypertonic solutions If two solutions have unequal
osmotic pressure, the more
concentrated solution with the
higher osmotic pressure is said to
be hypertonic
In a sucrose AND urea solution,
Sucrose Higher osmotic
pressureHypertonic
Hypotonic solutions If two solutions have unequal
osmotic pressure, the more dilute
solution with the lower osmotic
pressure is said to be hypertonic
In a sucrose AND urea solution,
Urea Lower osmotic
pressureHyptonic
Presented by: Freya Cardozo
67
Osmotic pressure and conc. Of solution
 For dilute solution the osmotic pressure can be given
by,
 V= volume of the solution in dm3
n2= number of moles of non volatile solute
R= real gas constant = 0.08206 dm3 atm K-1 mol-1
Π= Osmotic pressure in atm
Presented by: Freya Cardozo
68
 We know that Concentration= n2/V
 Concentration can be written in terms of
Molarity M
 Thus, equation becomes
 Here, we can use molarity instead of
molality because the osmotic pressures
are measured at a constant temperature.
Presented by: Freya Cardozo
69
Molar mass of solute from osmotic pressure
Presented by: Freya Cardozo
70
Reverse osmosis
 The direction of osmosis if from pure solvent to solution but
this can be reversed by applying a pressure higher than the
osmotic pressure
 The pure solvent then flows from solution into pure solvent
through semipermeable membrane. This is called reverse
osmosis.
 Eg. Fresh water and salty water separation using semipermeable
membrane
 On application of pressure higher than osmotic pressure, the
salty water passes into fresh pure water
 This leaves the salt behind
Presented by: Freya Cardozo
71
Presented by: Freya Cardozo
72
Colligative properties of electrolytes
1. The solutions of electrolytes also exhibit colligative properties which do not obey
the relations of non-electrolytes
2. The colligative properties of the solutions of electrolytes are greater than those to
be expected for solutions of non electrolytes of the same concentrations
3. The molar masses of electrolytes in aqueous solutions determined by colligative
properties are found to be considerably lower than the formula masses
Presented by: Freya Cardozo
73
Why is colligative properties of
electrolytes more than nonelectrolytes
Electrolytes-
Dissociates
Increases the
number of
particles
Increase in
colligative
particles
Eg. NaCl(lesser
C.P) Vs
Sucrose(more
C.P)
Presented by: Freya Cardozo
74
Van’t Hoff factor (i)
 In order to account for the dissociation/ association of electrolytes and to calculate their colligative
properties Van’t Hoff suggested the factor i
 It can be defined as the ratio of colligative property of a solution of electrolyte divided by the
colligative property of nonelectrolyte solution of the same concentration.
 No subscript  electrolyte solutions With subscript nonelectrolyte solutions
Presented by: Freya Cardozo
75
Definitions
 It is also defined as ,
Presented by: Freya Cardozo
76
i=2
KNO3
NaCl
i=3
CaCl2
Na2SO4
i=1 for non
electrolytic
solutions
Why colligative properties of higher
concentration solutions smaller than
expected?
 The electrostatic forces between the oppositely charged ions bring about the
formation of ion pairs
 Each ion pair consists of one or more cations and one or more anions held
together by electrostatic attractive forces
 This results in decrease in the number of particles in solution causing reduction in
the expected I value and colligative properties
Presented by: Freya Cardozo
77
Modifications of expressions of colligative
properties
Presented by: Freya Cardozo
78
Van’t Hoff factor i and degree of dissociation
 For weak electrolytes Dissociation is related tαo Degree of dissociation α
 Consider the equation
 Initially 1 mol 0 0
At equilibrium (1- α)mol x α y α
Total moles after dissociation = (1- α)+ x α + y α= 1+ α (x+y-1)= 1+ α(n-1) [Since, n=x+y]
Vant Hoff factor can thus be given by,
Presented by: Freya Cardozo
79
Presented by: Freya Cardozo
80
Presented by: Freya Cardozo
81
Presented by: Freya Cardozo
82

More Related Content

What's hot

Solutions and their types
Solutions and their typesSolutions and their types
Solutions and their types
International advisers
 
Class XI CH 2 (relations and functions)
Class XI CH 2 (relations and functions)Class XI CH 2 (relations and functions)
Class XI CH 2 (relations and functions)
Pradeep Sharma
 
4 Pius Augustine Density and Relative Density
4 Pius Augustine  Density and Relative Density4 Pius Augustine  Density and Relative Density
4 Pius Augustine Density and Relative Density
PiusAugustine
 
Chapter 2 mechanical properties of fluids
Chapter 2   mechanical properties of fluids Chapter 2   mechanical properties of fluids
Chapter 2 mechanical properties of fluids
Pooja M
 
Ionic equilibrium chapter 3(12th HSC Maharashtra state board)
Ionic equilibrium chapter 3(12th HSC Maharashtra state board)Ionic equilibrium chapter 3(12th HSC Maharashtra state board)
Ionic equilibrium chapter 3(12th HSC Maharashtra state board)
Freya Cardozo
 
Chemical equilibrium
Chemical equilibriumChemical equilibrium
Chemical equilibrium
Arunesh Gupta
 
divergence of vector and divergence theorem
divergence of vector and divergence theoremdivergence of vector and divergence theorem
divergence of vector and divergence theorem
AbhishekLalkiya
 
Dot & cross product of vectors
Dot & cross product of vectorsDot & cross product of vectors
Dot & cross product of vectors
Ashraful Tauhid
 
Colligative Properties Of Solutions
Colligative Properties Of SolutionsColligative Properties Of Solutions
Colligative Properties Of Solutions
cenglish5
 
Ch 03b motion in a plane
Ch 03b motion in a planeCh 03b motion in a plane
Ch 03b motion in a plane
Raghav Vasudeva
 
Ch 03b motion in a plane
Ch 03b motion in a planeCh 03b motion in a plane
Ch 03b motion in a plane
Raghav Vasudeva
 
Ppt on work energy and power class xi science
Ppt on work energy and power class xi sciencePpt on work energy and power class xi science
Ppt on work energy and power class xi science
acceleration gravity
 
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiationPHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
Pooja M
 
Surface chemistry, class xii
Surface chemistry, class  xiiSurface chemistry, class  xii
Surface chemistry, class xii
tanuja05
 
Chemical kinetics- Physical Chemistry
Chemical kinetics- Physical ChemistryChemical kinetics- Physical Chemistry
Chemical kinetics- Physical Chemistry
Sanchit Dhankhar
 
Kinetic theory of gases
Kinetic theory of gasesKinetic theory of gases
Kinetic theory of gases
Radha Mini
 
Motion in a plane
Motion in a planeMotion in a plane
Motion in a plane
VIDYAGAUDE
 
Pressure in fluids
Pressure in fluidsPressure in fluids
Pressure in fluidsreastment
 

What's hot (20)

Solutions and their types
Solutions and their typesSolutions and their types
Solutions and their types
 
Class XI CH 2 (relations and functions)
Class XI CH 2 (relations and functions)Class XI CH 2 (relations and functions)
Class XI CH 2 (relations and functions)
 
4 Pius Augustine Density and Relative Density
4 Pius Augustine  Density and Relative Density4 Pius Augustine  Density and Relative Density
4 Pius Augustine Density and Relative Density
 
Ratio line segment on parallel lines
Ratio line segment on parallel linesRatio line segment on parallel lines
Ratio line segment on parallel lines
 
Chapter 2 mechanical properties of fluids
Chapter 2   mechanical properties of fluids Chapter 2   mechanical properties of fluids
Chapter 2 mechanical properties of fluids
 
Ionic equilibrium chapter 3(12th HSC Maharashtra state board)
Ionic equilibrium chapter 3(12th HSC Maharashtra state board)Ionic equilibrium chapter 3(12th HSC Maharashtra state board)
Ionic equilibrium chapter 3(12th HSC Maharashtra state board)
 
Chemical equilibrium
Chemical equilibriumChemical equilibrium
Chemical equilibrium
 
Simple harmonic motion
Simple harmonic motionSimple harmonic motion
Simple harmonic motion
 
divergence of vector and divergence theorem
divergence of vector and divergence theoremdivergence of vector and divergence theorem
divergence of vector and divergence theorem
 
Dot & cross product of vectors
Dot & cross product of vectorsDot & cross product of vectors
Dot & cross product of vectors
 
Colligative Properties Of Solutions
Colligative Properties Of SolutionsColligative Properties Of Solutions
Colligative Properties Of Solutions
 
Ch 03b motion in a plane
Ch 03b motion in a planeCh 03b motion in a plane
Ch 03b motion in a plane
 
Ch 03b motion in a plane
Ch 03b motion in a planeCh 03b motion in a plane
Ch 03b motion in a plane
 
Ppt on work energy and power class xi science
Ppt on work energy and power class xi sciencePpt on work energy and power class xi science
Ppt on work energy and power class xi science
 
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiationPHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
PHYSICS CLASS XII Chapter 3 - Kinetic theory of gases and radiation
 
Surface chemistry, class xii
Surface chemistry, class  xiiSurface chemistry, class  xii
Surface chemistry, class xii
 
Chemical kinetics- Physical Chemistry
Chemical kinetics- Physical ChemistryChemical kinetics- Physical Chemistry
Chemical kinetics- Physical Chemistry
 
Kinetic theory of gases
Kinetic theory of gasesKinetic theory of gases
Kinetic theory of gases
 
Motion in a plane
Motion in a planeMotion in a plane
Motion in a plane
 
Pressure in fluids
Pressure in fluidsPressure in fluids
Pressure in fluids
 

Similar to Solution colligative properties 12th HSC Maharashtra state board

solutions.pdf
solutions.pdfsolutions.pdf
solutions.pdf
Renuha0130
 
3- Solutions & It's Colligative Properties(Physical Pharmacy)
3- Solutions & It's Colligative Properties(Physical Pharmacy)3- Solutions & It's Colligative Properties(Physical Pharmacy)
3- Solutions & It's Colligative Properties(Physical Pharmacy)
Rawa M. Ahmed
 
RAOULT'S LAW ( Physical & Analytical Chemistry)
RAOULT'S LAW ( Physical & Analytical Chemistry)RAOULT'S LAW ( Physical & Analytical Chemistry)
RAOULT'S LAW ( Physical & Analytical Chemistry)
Hasnaın Sheıkh
 
Colligative properties of dilute solutions Manik
Colligative properties of dilute solutions Manik Colligative properties of dilute solutions Manik
Colligative properties of dilute solutions Manik
Imran Nur Manik
 
Solutions of nonelectrolytes-Physical Pharmacy
Solutions of nonelectrolytes-Physical PharmacySolutions of nonelectrolytes-Physical Pharmacy
Solutions of nonelectrolytes-Physical Pharmacy
Dr Jayapal Reddy Gangadi
 
SOLUTIONS book 1 unit 1 class 12 ppt.pptx
SOLUTIONS book 1 unit 1 class 12 ppt.pptxSOLUTIONS book 1 unit 1 class 12 ppt.pptx
SOLUTIONS book 1 unit 1 class 12 ppt.pptx
vanshika2933
 
Solution & Colligative properties
Solution & Colligative propertiesSolution & Colligative properties
Solution & Colligative properties
NirmalaAnchigavi
 
1st Lecture on Solutions | Chemistry Part I | 12th Science
1st Lecture on Solutions | Chemistry Part I | 12th Science1st Lecture on Solutions | Chemistry Part I | 12th Science
1st Lecture on Solutions | Chemistry Part I | 12th Science
Ansari Usama
 
colligative Properties MANIK
colligative Properties MANIKcolligative Properties MANIK
colligative Properties MANIK
Imran Nur Manik
 
Chemistry
Chemistry Chemistry
Chemistry
GAMELORD3
 
Solution.pdf
Solution.pdfSolution.pdf
Solution.pdf
LUXMIKANTGIRI
 
solutionchemistry-.pdf
solutionchemistry-.pdfsolutionchemistry-.pdf
solutionchemistry-.pdf
LUXMIKANTGIRI
 
solution class12.pptx
solution class12.pptxsolution class12.pptx
solution class12.pptx
niralipatil
 
CBSE Class 12 Chemistry Chapter 2 (Solutions) | Homi Institute
CBSE Class 12 Chemistry Chapter 2 (Solutions) | Homi InstituteCBSE Class 12 Chemistry Chapter 2 (Solutions) | Homi Institute
CBSE Class 12 Chemistry Chapter 2 (Solutions) | Homi Institute
Homi Institute
 
chem2.pptx
chem2.pptxchem2.pptx
chem2.pptx
DheerajPrajapati34
 
Hsslive-xii-chem-slide-ch-2.Solutions.pdf
Hsslive-xii-chem-slide-ch-2.Solutions.pdfHsslive-xii-chem-slide-ch-2.Solutions.pdf
Hsslive-xii-chem-slide-ch-2.Solutions.pdf
jayanethaji
 
CHEMISTRYBOOKSECONDCOPYNOTAALLOWEDAF.ppt
CHEMISTRYBOOKSECONDCOPYNOTAALLOWEDAF.pptCHEMISTRYBOOKSECONDCOPYNOTAALLOWEDAF.ppt
CHEMISTRYBOOKSECONDCOPYNOTAALLOWEDAF.ppt
GuptaKira1
 
Chemistry chapter 1 solutions detailed explanation
Chemistry chapter 1 solutions detailed explanationChemistry chapter 1 solutions detailed explanation
Chemistry chapter 1 solutions detailed explanation
ayuqroyjohn85
 
SOLUTIONS_ppt_1_1.pptx
SOLUTIONS_ppt_1_1.pptxSOLUTIONS_ppt_1_1.pptx
SOLUTIONS_ppt_1_1.pptx
CSKrithik
 
DOC-20230413-WA0000.pptx
DOC-20230413-WA0000.pptxDOC-20230413-WA0000.pptx
DOC-20230413-WA0000.pptx
SachinYadav923245
 

Similar to Solution colligative properties 12th HSC Maharashtra state board (20)

solutions.pdf
solutions.pdfsolutions.pdf
solutions.pdf
 
3- Solutions & It's Colligative Properties(Physical Pharmacy)
3- Solutions & It's Colligative Properties(Physical Pharmacy)3- Solutions & It's Colligative Properties(Physical Pharmacy)
3- Solutions & It's Colligative Properties(Physical Pharmacy)
 
RAOULT'S LAW ( Physical & Analytical Chemistry)
RAOULT'S LAW ( Physical & Analytical Chemistry)RAOULT'S LAW ( Physical & Analytical Chemistry)
RAOULT'S LAW ( Physical & Analytical Chemistry)
 
Colligative properties of dilute solutions Manik
Colligative properties of dilute solutions Manik Colligative properties of dilute solutions Manik
Colligative properties of dilute solutions Manik
 
Solutions of nonelectrolytes-Physical Pharmacy
Solutions of nonelectrolytes-Physical PharmacySolutions of nonelectrolytes-Physical Pharmacy
Solutions of nonelectrolytes-Physical Pharmacy
 
SOLUTIONS book 1 unit 1 class 12 ppt.pptx
SOLUTIONS book 1 unit 1 class 12 ppt.pptxSOLUTIONS book 1 unit 1 class 12 ppt.pptx
SOLUTIONS book 1 unit 1 class 12 ppt.pptx
 
Solution & Colligative properties
Solution & Colligative propertiesSolution & Colligative properties
Solution & Colligative properties
 
1st Lecture on Solutions | Chemistry Part I | 12th Science
1st Lecture on Solutions | Chemistry Part I | 12th Science1st Lecture on Solutions | Chemistry Part I | 12th Science
1st Lecture on Solutions | Chemistry Part I | 12th Science
 
colligative Properties MANIK
colligative Properties MANIKcolligative Properties MANIK
colligative Properties MANIK
 
Chemistry
Chemistry Chemistry
Chemistry
 
Solution.pdf
Solution.pdfSolution.pdf
Solution.pdf
 
solutionchemistry-.pdf
solutionchemistry-.pdfsolutionchemistry-.pdf
solutionchemistry-.pdf
 
solution class12.pptx
solution class12.pptxsolution class12.pptx
solution class12.pptx
 
CBSE Class 12 Chemistry Chapter 2 (Solutions) | Homi Institute
CBSE Class 12 Chemistry Chapter 2 (Solutions) | Homi InstituteCBSE Class 12 Chemistry Chapter 2 (Solutions) | Homi Institute
CBSE Class 12 Chemistry Chapter 2 (Solutions) | Homi Institute
 
chem2.pptx
chem2.pptxchem2.pptx
chem2.pptx
 
Hsslive-xii-chem-slide-ch-2.Solutions.pdf
Hsslive-xii-chem-slide-ch-2.Solutions.pdfHsslive-xii-chem-slide-ch-2.Solutions.pdf
Hsslive-xii-chem-slide-ch-2.Solutions.pdf
 
CHEMISTRYBOOKSECONDCOPYNOTAALLOWEDAF.ppt
CHEMISTRYBOOKSECONDCOPYNOTAALLOWEDAF.pptCHEMISTRYBOOKSECONDCOPYNOTAALLOWEDAF.ppt
CHEMISTRYBOOKSECONDCOPYNOTAALLOWEDAF.ppt
 
Chemistry chapter 1 solutions detailed explanation
Chemistry chapter 1 solutions detailed explanationChemistry chapter 1 solutions detailed explanation
Chemistry chapter 1 solutions detailed explanation
 
SOLUTIONS_ppt_1_1.pptx
SOLUTIONS_ppt_1_1.pptxSOLUTIONS_ppt_1_1.pptx
SOLUTIONS_ppt_1_1.pptx
 
DOC-20230413-WA0000.pptx
DOC-20230413-WA0000.pptxDOC-20230413-WA0000.pptx
DOC-20230413-WA0000.pptx
 

More from Freya Cardozo

Hardy Weinberg law
Hardy Weinberg lawHardy Weinberg law
Hardy Weinberg law
Freya Cardozo
 
Evolution- Natural selection and Genetic Drift and modes of natural selection
Evolution- Natural selection and Genetic Drift and modes of natural selectionEvolution- Natural selection and Genetic Drift and modes of natural selection
Evolution- Natural selection and Genetic Drift and modes of natural selection
Freya Cardozo
 
Patterns of speciation- Allopatric, Sympatric, Parapatric and Peripatric
Patterns of speciation- Allopatric, Sympatric, Parapatric and PeripatricPatterns of speciation- Allopatric, Sympatric, Parapatric and Peripatric
Patterns of speciation- Allopatric, Sympatric, Parapatric and Peripatric
Freya Cardozo
 
Molecular clock, Neutral hypothesis
Molecular clock, Neutral hypothesisMolecular clock, Neutral hypothesis
Molecular clock, Neutral hypothesis
Freya Cardozo
 
Altrusim and Hamilton rule
Altrusim and Hamilton ruleAltrusim and Hamilton rule
Altrusim and Hamilton rule
Freya Cardozo
 
Flowering in plants(Arabidopsis) ABC Model
Flowering in plants(Arabidopsis) ABC ModelFlowering in plants(Arabidopsis) ABC Model
Flowering in plants(Arabidopsis) ABC Model
Freya Cardozo
 
FACS Flow cytometry| Apoptosis & Necrosis| CSIR NET SET Questions
FACS Flow cytometry| Apoptosis & Necrosis| CSIR NET SET QuestionsFACS Flow cytometry| Apoptosis & Necrosis| CSIR NET SET Questions
FACS Flow cytometry| Apoptosis & Necrosis| CSIR NET SET Questions
Freya Cardozo
 
Synthesis of oligonucleotides by phosphoramidite method
Synthesis of oligonucleotides by phosphoramidite methodSynthesis of oligonucleotides by phosphoramidite method
Synthesis of oligonucleotides by phosphoramidite method
Freya Cardozo
 
Pullulan- Industrially Important Biopolymer(Exopolysaccharide)
Pullulan- Industrially Important Biopolymer(Exopolysaccharide)Pullulan- Industrially Important Biopolymer(Exopolysaccharide)
Pullulan- Industrially Important Biopolymer(Exopolysaccharide)
Freya Cardozo
 
IMViC Biochemical Tests Principle|Indole|Methyl Red|Voges Proskauer|Citrate Test
IMViC Biochemical Tests Principle|Indole|Methyl Red|Voges Proskauer|Citrate TestIMViC Biochemical Tests Principle|Indole|Methyl Red|Voges Proskauer|Citrate Test
IMViC Biochemical Tests Principle|Indole|Methyl Red|Voges Proskauer|Citrate Test
Freya Cardozo
 
Nuclear chemistry and radioactivity
Nuclear chemistry and radioactivityNuclear chemistry and radioactivity
Nuclear chemistry and radioactivity
Freya Cardozo
 
Halogen derivates of alkanes HDA
Halogen derivates of alkanes HDAHalogen derivates of alkanes HDA
Halogen derivates of alkanes HDA
Freya Cardozo
 
Nuclear chemistry and radioactivity
Nuclear chemistry and radioactivityNuclear chemistry and radioactivity
Nuclear chemistry and radioactivity
Freya Cardozo
 
Some basic concepts of chemistry
Some basic concepts of chemistrySome basic concepts of chemistry
Some basic concepts of chemistry
Freya Cardozo
 
Coordination compounds (12th Maharashtra state board)
Coordination compounds (12th Maharashtra state board)Coordination compounds (12th Maharashtra state board)
Coordination compounds (12th Maharashtra state board)
Freya Cardozo
 
Structure of atom(11th standard Maharashtra state board)
Structure of atom(11th standard Maharashtra state board)Structure of atom(11th standard Maharashtra state board)
Structure of atom(11th standard Maharashtra state board)
Freya Cardozo
 
Biological membranes as a barriers to drugs(pH trapping)
Biological membranes as a barriers to drugs(pH trapping)Biological membranes as a barriers to drugs(pH trapping)
Biological membranes as a barriers to drugs(pH trapping)
Freya Cardozo
 
HPV vaccine (UID198612)
HPV vaccine (UID198612)HPV vaccine (UID198612)
HPV vaccine (UID198612)
Freya Cardozo
 
d and f block elements/Transition and inner transition elements
d and f block elements/Transition and inner transition elementsd and f block elements/Transition and inner transition elements
d and f block elements/Transition and inner transition elements
Freya Cardozo
 
Polymers 12th State Board
Polymers 12th State BoardPolymers 12th State Board
Polymers 12th State Board
Freya Cardozo
 

More from Freya Cardozo (20)

Hardy Weinberg law
Hardy Weinberg lawHardy Weinberg law
Hardy Weinberg law
 
Evolution- Natural selection and Genetic Drift and modes of natural selection
Evolution- Natural selection and Genetic Drift and modes of natural selectionEvolution- Natural selection and Genetic Drift and modes of natural selection
Evolution- Natural selection and Genetic Drift and modes of natural selection
 
Patterns of speciation- Allopatric, Sympatric, Parapatric and Peripatric
Patterns of speciation- Allopatric, Sympatric, Parapatric and PeripatricPatterns of speciation- Allopatric, Sympatric, Parapatric and Peripatric
Patterns of speciation- Allopatric, Sympatric, Parapatric and Peripatric
 
Molecular clock, Neutral hypothesis
Molecular clock, Neutral hypothesisMolecular clock, Neutral hypothesis
Molecular clock, Neutral hypothesis
 
Altrusim and Hamilton rule
Altrusim and Hamilton ruleAltrusim and Hamilton rule
Altrusim and Hamilton rule
 
Flowering in plants(Arabidopsis) ABC Model
Flowering in plants(Arabidopsis) ABC ModelFlowering in plants(Arabidopsis) ABC Model
Flowering in plants(Arabidopsis) ABC Model
 
FACS Flow cytometry| Apoptosis & Necrosis| CSIR NET SET Questions
FACS Flow cytometry| Apoptosis & Necrosis| CSIR NET SET QuestionsFACS Flow cytometry| Apoptosis & Necrosis| CSIR NET SET Questions
FACS Flow cytometry| Apoptosis & Necrosis| CSIR NET SET Questions
 
Synthesis of oligonucleotides by phosphoramidite method
Synthesis of oligonucleotides by phosphoramidite methodSynthesis of oligonucleotides by phosphoramidite method
Synthesis of oligonucleotides by phosphoramidite method
 
Pullulan- Industrially Important Biopolymer(Exopolysaccharide)
Pullulan- Industrially Important Biopolymer(Exopolysaccharide)Pullulan- Industrially Important Biopolymer(Exopolysaccharide)
Pullulan- Industrially Important Biopolymer(Exopolysaccharide)
 
IMViC Biochemical Tests Principle|Indole|Methyl Red|Voges Proskauer|Citrate Test
IMViC Biochemical Tests Principle|Indole|Methyl Red|Voges Proskauer|Citrate TestIMViC Biochemical Tests Principle|Indole|Methyl Red|Voges Proskauer|Citrate Test
IMViC Biochemical Tests Principle|Indole|Methyl Red|Voges Proskauer|Citrate Test
 
Nuclear chemistry and radioactivity
Nuclear chemistry and radioactivityNuclear chemistry and radioactivity
Nuclear chemistry and radioactivity
 
Halogen derivates of alkanes HDA
Halogen derivates of alkanes HDAHalogen derivates of alkanes HDA
Halogen derivates of alkanes HDA
 
Nuclear chemistry and radioactivity
Nuclear chemistry and radioactivityNuclear chemistry and radioactivity
Nuclear chemistry and radioactivity
 
Some basic concepts of chemistry
Some basic concepts of chemistrySome basic concepts of chemistry
Some basic concepts of chemistry
 
Coordination compounds (12th Maharashtra state board)
Coordination compounds (12th Maharashtra state board)Coordination compounds (12th Maharashtra state board)
Coordination compounds (12th Maharashtra state board)
 
Structure of atom(11th standard Maharashtra state board)
Structure of atom(11th standard Maharashtra state board)Structure of atom(11th standard Maharashtra state board)
Structure of atom(11th standard Maharashtra state board)
 
Biological membranes as a barriers to drugs(pH trapping)
Biological membranes as a barriers to drugs(pH trapping)Biological membranes as a barriers to drugs(pH trapping)
Biological membranes as a barriers to drugs(pH trapping)
 
HPV vaccine (UID198612)
HPV vaccine (UID198612)HPV vaccine (UID198612)
HPV vaccine (UID198612)
 
d and f block elements/Transition and inner transition elements
d and f block elements/Transition and inner transition elementsd and f block elements/Transition and inner transition elements
d and f block elements/Transition and inner transition elements
 
Polymers 12th State Board
Polymers 12th State BoardPolymers 12th State Board
Polymers 12th State Board
 

Recently uploaded

Polish students' mobility in the Czech Republic
Polish students' mobility in the Czech RepublicPolish students' mobility in the Czech Republic
Polish students' mobility in the Czech Republic
Anna Sz.
 
Chapter 3 - Islamic Banking Products and Services.pptx
Chapter 3 - Islamic Banking Products and Services.pptxChapter 3 - Islamic Banking Products and Services.pptx
Chapter 3 - Islamic Banking Products and Services.pptx
Mohd Adib Abd Muin, Senior Lecturer at Universiti Utara Malaysia
 
aaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaa
aaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaa
aaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaa
siemaillard
 
The approach at University of Liverpool.pptx
The approach at University of Liverpool.pptxThe approach at University of Liverpool.pptx
The approach at University of Liverpool.pptx
Jisc
 
Adversarial Attention Modeling for Multi-dimensional Emotion Regression.pdf
Adversarial Attention Modeling for Multi-dimensional Emotion Regression.pdfAdversarial Attention Modeling for Multi-dimensional Emotion Regression.pdf
Adversarial Attention Modeling for Multi-dimensional Emotion Regression.pdf
Po-Chuan Chen
 
Francesca Gottschalk - How can education support child empowerment.pptx
Francesca Gottschalk - How can education support child empowerment.pptxFrancesca Gottschalk - How can education support child empowerment.pptx
Francesca Gottschalk - How can education support child empowerment.pptx
EduSkills OECD
 
Sha'Carri Richardson Presentation 202345
Sha'Carri Richardson Presentation 202345Sha'Carri Richardson Presentation 202345
Sha'Carri Richardson Presentation 202345
beazzy04
 
special B.ed 2nd year old paper_20240531.pdf
special B.ed 2nd year old paper_20240531.pdfspecial B.ed 2nd year old paper_20240531.pdf
special B.ed 2nd year old paper_20240531.pdf
Special education needs
 
Instructions for Submissions thorugh G- Classroom.pptx
Instructions for Submissions thorugh G- Classroom.pptxInstructions for Submissions thorugh G- Classroom.pptx
Instructions for Submissions thorugh G- Classroom.pptx
Jheel Barad
 
Additional Benefits for Employee Website.pdf
Additional Benefits for Employee Website.pdfAdditional Benefits for Employee Website.pdf
Additional Benefits for Employee Website.pdf
joachimlavalley1
 
Digital Tools and AI for Teaching Learning and Research
Digital Tools and AI for Teaching Learning and ResearchDigital Tools and AI for Teaching Learning and Research
Digital Tools and AI for Teaching Learning and Research
Vikramjit Singh
 
Biological Screening of Herbal Drugs in detailed.
Biological Screening of Herbal Drugs in detailed.Biological Screening of Herbal Drugs in detailed.
Biological Screening of Herbal Drugs in detailed.
Ashokrao Mane college of Pharmacy Peth-Vadgaon
 
Introduction to AI for Nonprofits with Tapp Network
Introduction to AI for Nonprofits with Tapp NetworkIntroduction to AI for Nonprofits with Tapp Network
Introduction to AI for Nonprofits with Tapp Network
TechSoup
 
Unit 8 - Information and Communication Technology (Paper I).pdf
Unit 8 - Information and Communication Technology (Paper I).pdfUnit 8 - Information and Communication Technology (Paper I).pdf
Unit 8 - Information and Communication Technology (Paper I).pdf
Thiyagu K
 
The Accursed House by Émile Gaboriau.pptx
The Accursed House by Émile Gaboriau.pptxThe Accursed House by Émile Gaboriau.pptx
The Accursed House by Émile Gaboriau.pptx
DhatriParmar
 
Lapbook sobre os Regimes Totalitários.pdf
Lapbook sobre os Regimes Totalitários.pdfLapbook sobre os Regimes Totalitários.pdf
Lapbook sobre os Regimes Totalitários.pdf
Jean Carlos Nunes Paixão
 
How libraries can support authors with open access requirements for UKRI fund...
How libraries can support authors with open access requirements for UKRI fund...How libraries can support authors with open access requirements for UKRI fund...
How libraries can support authors with open access requirements for UKRI fund...
Jisc
 
The French Revolution Class 9 Study Material pdf free download
The French Revolution Class 9 Study Material pdf free downloadThe French Revolution Class 9 Study Material pdf free download
The French Revolution Class 9 Study Material pdf free download
Vivekanand Anglo Vedic Academy
 
The Roman Empire A Historical Colossus.pdf
The Roman Empire A Historical Colossus.pdfThe Roman Empire A Historical Colossus.pdf
The Roman Empire A Historical Colossus.pdf
kaushalkr1407
 
CLASS 11 CBSE B.St Project AIDS TO TRADE - INSURANCE
CLASS 11 CBSE B.St Project AIDS TO TRADE - INSURANCECLASS 11 CBSE B.St Project AIDS TO TRADE - INSURANCE
CLASS 11 CBSE B.St Project AIDS TO TRADE - INSURANCE
BhavyaRajput3
 

Recently uploaded (20)

Polish students' mobility in the Czech Republic
Polish students' mobility in the Czech RepublicPolish students' mobility in the Czech Republic
Polish students' mobility in the Czech Republic
 
Chapter 3 - Islamic Banking Products and Services.pptx
Chapter 3 - Islamic Banking Products and Services.pptxChapter 3 - Islamic Banking Products and Services.pptx
Chapter 3 - Islamic Banking Products and Services.pptx
 
aaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaa
aaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaa
aaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaa
 
The approach at University of Liverpool.pptx
The approach at University of Liverpool.pptxThe approach at University of Liverpool.pptx
The approach at University of Liverpool.pptx
 
Adversarial Attention Modeling for Multi-dimensional Emotion Regression.pdf
Adversarial Attention Modeling for Multi-dimensional Emotion Regression.pdfAdversarial Attention Modeling for Multi-dimensional Emotion Regression.pdf
Adversarial Attention Modeling for Multi-dimensional Emotion Regression.pdf
 
Francesca Gottschalk - How can education support child empowerment.pptx
Francesca Gottschalk - How can education support child empowerment.pptxFrancesca Gottschalk - How can education support child empowerment.pptx
Francesca Gottschalk - How can education support child empowerment.pptx
 
Sha'Carri Richardson Presentation 202345
Sha'Carri Richardson Presentation 202345Sha'Carri Richardson Presentation 202345
Sha'Carri Richardson Presentation 202345
 
special B.ed 2nd year old paper_20240531.pdf
special B.ed 2nd year old paper_20240531.pdfspecial B.ed 2nd year old paper_20240531.pdf
special B.ed 2nd year old paper_20240531.pdf
 
Instructions for Submissions thorugh G- Classroom.pptx
Instructions for Submissions thorugh G- Classroom.pptxInstructions for Submissions thorugh G- Classroom.pptx
Instructions for Submissions thorugh G- Classroom.pptx
 
Additional Benefits for Employee Website.pdf
Additional Benefits for Employee Website.pdfAdditional Benefits for Employee Website.pdf
Additional Benefits for Employee Website.pdf
 
Digital Tools and AI for Teaching Learning and Research
Digital Tools and AI for Teaching Learning and ResearchDigital Tools and AI for Teaching Learning and Research
Digital Tools and AI for Teaching Learning and Research
 
Biological Screening of Herbal Drugs in detailed.
Biological Screening of Herbal Drugs in detailed.Biological Screening of Herbal Drugs in detailed.
Biological Screening of Herbal Drugs in detailed.
 
Introduction to AI for Nonprofits with Tapp Network
Introduction to AI for Nonprofits with Tapp NetworkIntroduction to AI for Nonprofits with Tapp Network
Introduction to AI for Nonprofits with Tapp Network
 
Unit 8 - Information and Communication Technology (Paper I).pdf
Unit 8 - Information and Communication Technology (Paper I).pdfUnit 8 - Information and Communication Technology (Paper I).pdf
Unit 8 - Information and Communication Technology (Paper I).pdf
 
The Accursed House by Émile Gaboriau.pptx
The Accursed House by Émile Gaboriau.pptxThe Accursed House by Émile Gaboriau.pptx
The Accursed House by Émile Gaboriau.pptx
 
Lapbook sobre os Regimes Totalitários.pdf
Lapbook sobre os Regimes Totalitários.pdfLapbook sobre os Regimes Totalitários.pdf
Lapbook sobre os Regimes Totalitários.pdf
 
How libraries can support authors with open access requirements for UKRI fund...
How libraries can support authors with open access requirements for UKRI fund...How libraries can support authors with open access requirements for UKRI fund...
How libraries can support authors with open access requirements for UKRI fund...
 
The French Revolution Class 9 Study Material pdf free download
The French Revolution Class 9 Study Material pdf free downloadThe French Revolution Class 9 Study Material pdf free download
The French Revolution Class 9 Study Material pdf free download
 
The Roman Empire A Historical Colossus.pdf
The Roman Empire A Historical Colossus.pdfThe Roman Empire A Historical Colossus.pdf
The Roman Empire A Historical Colossus.pdf
 
CLASS 11 CBSE B.St Project AIDS TO TRADE - INSURANCE
CLASS 11 CBSE B.St Project AIDS TO TRADE - INSURANCECLASS 11 CBSE B.St Project AIDS TO TRADE - INSURANCE
CLASS 11 CBSE B.St Project AIDS TO TRADE - INSURANCE
 

Solution colligative properties 12th HSC Maharashtra state board

  • 2. Solution  It is a homogenous mixture of two or more pure substances  Solution= Solute + Solvent  Solvent is the one present in larger quantity  Solute is the one present in smaller quantities  Solutions with only one solute are called Binary solutions Presented by: Freya Cardozo 2
  • 3. Types of solutions  The solute and solvent can be in any of the following state solids, liquids or gases  Combinations of these gives mainly 9 types of solutions Presented by: Freya Cardozo 3
  • 5. Solubility  The solubility of a solute is its amount per unit volume of saturated solution at a specific temperature  Solubility unit= mol L-1 Presented by: Freya Cardozo 5
  • 6. Factors affecting solubility  Nature of solute and solvent  Effect of temperature on solubility  Effect of pressure on solubility Presented by: Freya Cardozo 6
  • 7. Nature of solute and solvent  Like dissolves like  Similar chemical character are more readily soluble in each other than different chemical natures  Similar substances also have similar intermolecular forces of attraction  Polar solutes dissolve in polar solvents because , solute-solute, Solute- solvent and solvent-solvent interactions are of similar magnitude  Eg. NaCl in water, Cholesterol in Benzene, Sugar in water Presented by: Freya Cardozo 7
  • 8. Effect of temperature on solubility  For endothermic processes – Eg. KCl in water ↑T ↑Solubility because there is an increase in stress on the solution  For exothermic process – CaCl2 in water ↑T ↓Solubility But there hasn’t been any direct relation between exo and endothermicity on T Presented by: Freya Cardozo 8
  • 9. T Vs Solubility  NaBr, NaCl, KCl : S slightly changes with T  KNO3, NaNO3, KBr: ↑T ↑Solubility  Na2SO4 ↑T ↓Solubility Gas molecules are condensed in liquid phase, this process is exothermic. Thus, Solubility of gases in water should decreases with increase in temperature. Presented by: Freya Cardozo 9
  • 10. REAL LIFE EXAMPLE Industries take billions of gallons of water from rivers and lakes to cool down the equipment's which get heated during the industrial production process. Once the cool water is used the hot water produced is the returned to the water bodies again. Due to the increase in the temperature of water the solubility of gas in water decrease and thus it is very less available for fishes Presented by: Freya Cardozo 10
  • 11. Effect of pressure on solubility  Pressure has no effect on solubility of liquids and solids as they are incompressible  But for gases the solubility is greatly influenced by pressure  The relation between P and S for gases can be given by HENRY’S LAW Presented by: Freya Cardozo 11
  • 12. HENRY’S LAW  The law states that the solubility of a gas in a liquid is directly proportional to the pressure of the gas over the solution   Where, S= Solubilty of gase in molL-1 P=Pressure of gas over solution in bar KH= Henry constant. Unit is mol L-1 bar-1  When, P=1, KH=S. Thus, KH is the solubility of the gas in a liquid when its pressure over solution is 1 bae Presented by: Freya Cardozo 12
  • 13. Example and Exceptions  CO2 added in cold drinks under a pressure  As compared to normal conditions under pressure the solubility is much higher  Release relives this pressure giving the effervescence  Exceptions are NH3 and CO2 because they react with water  As they form these compounds they have higher solubilities than expected by Henrys law Presented by: Freya Cardozo 13
  • 14. Type 1 numericals  Based on Henry’s law  S=KHP Presented by: Freya Cardozo 14
  • 15. QUESTION  The henry’s law constant of CH3Br is 0.159 mol L-1 bar-1 at 250C. What is the solubility of CH3Br in water at 250C and at 130mm Hg? (1mmHg= 0.00133 bar) Presented by: Freya Cardozo 15
  • 16. RAOULT’S LAW  The law states that, “ The partial vapour pressure of any volatile component of a solution is equal to the vapour pressure of the pure component multiplied by its mole fraction in the solution.”  P= x P0  P= partial pressure  p0= partial pressure of pure component  x= mole fraction Presented by: Freya Cardozo 16
  • 17. Mole fraction  Mole fraction represents the number of molecules of a particular component in a mixture divided by the total number of moles in the given mixture. It's a way of expressing the concentration of a solution  Represented by x  The mole fraction of solute is x2 and solvent is x1; x1+x2=1 Presented by: Freya Cardozo 17
  • 18. Derive Raoult’s law 1. Let A1 and A2 be two volatile liquids, P1 and P2 be the respective partial pressures and P1 0 , P2 0 be vapour pressures of pure liquids 2. Let x1 and x2 be the mole fractions of A1 and A2 respectively 3. Raoult’s law can be written as P1= x1 P1 0 and P2 = x2 P2 0 Presented by: Freya Cardozo 18
  • 19. Since, P1 0 and P2 0 are constant P Vs x2 is a straight line P1 Vs X1 and P2 Vs x2 are also straight line passing through the origin Presented by: Freya Cardozo 19
  • 20. IDEAL SOLTIONS NONIDEAL SOLUTIONS 1. Obey Raoult’s law over entire range of concentrations 2. V.P always lies between V.P of pure components 3. No heat is evolved/ absorbed when 2 components are mixed. Enthalpy of mixing is zero. ∆mix H=0 4. No volume change. Thus Vol of sol. Is equal to sums of volumes of the 2 components mixed. ∆mixV=0 5. Solvent-solute, solute-solute and solvent-solvent molecular interactions are comparable 1. Do not obey Raoult’s law over entire range of concentrations 2. V.P of these solutions can be higher or lower than those of pure components 3. It shows two types of deviation:  Positive deviation  Negative deviation Presented by: Freya Cardozo 20
  • 21. POSITIVE DEVIATION NEGATIVE DEVIATION  Solute-solvent I.F.A (weaker)< solute-solute I.F.A & solvent-solvent I.F.A  V.P is higher than the pure components  Eg. Acetone+ Ethanol Acetone+ carbon disulphide  Solute-solvent I.F.A (stronger)> solute-solute I.F.A & solvent-solvent I.F.A  V.P is higher than the pure components  Eg. Acetone + chloroform Phenol + Aniline Presented by: Freya Cardozo 21 I.F.A= Intermolecular forces of attraction
  • 22. Colligative properties  Definition of colligative properties The physical properties of solutions that depend on the number of solute particles in solutions and not on their nature are called colligative properties  There are 4 colligative properties 1. Vapour pressure lowering 2. Boiling point elevation 3. Freezing point depression 4. osmotic pressure  Non-electrolytic and dilute solutions are used Presented by: Freya Cardozo 22
  • 23. Vapor pressure  The pressure exerted by the liquid vapor over the surface of a liquid in a closed container when both are in equilibrium is called as vapor pressure Presented by: Freya Cardozo 23
  • 24. VOLATILE SUBSTANCE NON-VOLATILE SUBSTANCE Presented by: Freya Cardozo 24
  • 25. Vapour pressure lowering  When a non volatile non-ionizable solid is dissolved in a liquid solvent, the vapour pressure of the solution is lower than that of the solvent.  If the solute is non-volatile it does not contribute to the VP above the solution  Thus VP of solution=VP of solvent above the solution  Mathematically, If P1 0 is the VP of pure solvent and P1 is the VP of solvent above the solution, P1< P1 0  Thus, vapour pressure lowering is ∆= P1 0 – P1 Presented by: Freya Cardozo 25
  • 26. Reason for this?  The vapour pressure of a liquid depends on the ease with which the molecules escape from the surface of liquid  When non-volatile solute is added it replaces some of the volatile solvent molecules at the surface and these non volatile solutes do not vaporizes and thus do not contribute to the vapour pressure.  Therefore, the number of solvent molecules available for vaporization per unit surface area is less than number at surface of pure solvent Presented by: Freya Cardozo 26
  • 27. Raoult’s law for solution of non volatile solutes OR Prove that ∆P= P1 0 x2 OR Prove lowering of vapour pressure is a colligative property  For a solution containing non volatile solute, the vapour pressure of solvent over the solution is equal to the vapour pressure multiplied by its mole fraction in the solution P1= P1 0 x1  For a binary solution containing 1 solute, x1=1-x2 (Since, x1+x2=1)  But, we know that lowering of vapour pressure is given by ∆= P1 0 – P1  Thus, ∆P= P1 0x2  From the above equation it is clear that the ∆P depends on x2 which is number of solute particles, thus lowering of vapour pressure is a colligative property Presented by: Freya Cardozo 27
  • 28. Relative Lowering of Vapour pressure  The ratio of vapour pressure lowering of solvent divided by the vapour pressure of pure solvent is called relative lowering of vapour pressure.  Thus,  Relative lowering of VP is equal to the mole fraction of solute in the solution. Therefore, relative lowering of VP is also a colligative property Presented by: Freya Cardozo 28
  • 29. Relationship between molar mass of solute and lowering of vapour pressure  We know that relative lowering of vapour pressure is equal to mole fraction of solute i.e.  The mole fraction of a component of solution is equal to its moles divided by the total moles in the solution. Thus,  n1= moles of solvent and n2= moles of solute  In dilute solutions, n1>>n2, thus n1+n2~n1.  Thus the mole fraction is Presented by: Freya Cardozo 29
  • 30.  Suppose a solution is prepared by adding W2 g of solute in W1 g of solvent. The moles of solute and solvent in the solution are,  Where, M1 and M2 are molar masses of solvent and solute respectively. Substituting in the equation, Presented by: Freya Cardozo 30
  • 31. WHAT DO YOU THINK? Presented by: Freya Cardozo 31
  • 32. TYPE 2 numericals ∆P= P1 0X2 Presented by: Freya Cardozo 32
  • 33. Presented by: Freya Cardozo 33In an experiment, 18.04 g of mannitol was dissolved in 100 g of water. The vapour pressure of water was lowered by 0.309 mm Hg from 17.535 mmHg. Calculate the molar mass of mannitol
  • 34. Presented by: Freya Cardozo 34 A solution is prepared by dissolving 394g of a non volatile solute is 622g of water. The vapour pressure of solution is found be 30.74 mm Hg at 300C. If the vapour pressure at 300C is 31.8 mm Hg, what is the molar mass of solute?
  • 35. Presented by: Freya Cardozo 35The vapour pressure of pure benzene (molar mass 78 g/mol) at a certain temperature is 640 mmHg. A non-volatile solute of mass 2.315g is added to 49g of benzene. Th vapour pressure of solution is 600 mmHg. What is the molar mass of the solute?
  • 36. Presented by: Freya Cardozo 36
  • 37. Boiling point elevation  B.P : The temperature at which the vapour pressure equals to the applied pressure/ atmospheric pressure(if open container)  Solutions with non volatile solute have higher B.P than pure solvent  If Tb 0 is B.P of pure solvent and Tb is of the solution then the difference between them ∆Tb  The difference between the B.P of solution and that of the pure solvent at any given point is called the boiling point elevation Presented by: Freya Cardozo 37
  • 38. Lowering of V.P and Elevation in B.P 1. In the graph Vapour pressure of the solvent and solution are plotted as a function of temperature 2. From the previous discussions we know that the vapour pressure of solution with non volatile solute<vapour pressure of pure solvent 3. Thus from graph we can see that CD= vapour pressure of solution(lower curve) AB= vapour pressure of pure solvent(higher curve) 4. The V.P difference goes on increasing with temperature Presented by: Freya Cardozo 38
  • 39. 5. The intersection of the curves AB and CD on the X axis shows that the boiling point of solution is more than the pure solvent 6. A liquid boils when its V.P is equal to 1 atm(atmospheric pressure). Therefore, in order for the solution to boil a higher temperature will be needed to reach 1 tm than the solvent. 7. That’s why the solution needs to be heated more to be boiled. Hence, there will be elevation in the B.P of solution even though there is a lowering of vapour pressure. [V.P is inversely related to B.P] Presented by: Freya Cardozo 39
  • 41. B.P elevation and conc. Of solute 1. The B.P elevation is directly proportional to molality of the solution. 2. Where, m= molality of solution Kb= boiling point elevation constant/ molal elevation constant/ ebullioscopic constant 3. If, m=1, ∆Tb=Kb Thus, ebullioscopic constant is the B.P elevation produced by 1 molal solution Presented by: Freya Cardozo 41
  • 43. Why molality over molarity? Because, we are studying systems where temperature is not constant thus we have to choose terms that do not depend on temperature molality is temperature independent whereas molarity depends on temperature This can be seen from the units also Presented by: Freya Cardozo 43 Molality= mol/kg Molarity= mol/L
  • 44. Relationship between mass of solute and boiling point elevation  Suppose a solution is made by dissolving W2 g of solute in W1 g of solvent  Moles of solute in solvent= W2/ M2 (M2= molar mass) Mass of solvent= W1g = W1 g/ 1000 g/kg = W1/ 1000 kg  Molality can be given by Presented by: Freya Cardozo 44
  • 45. TYPE 3: Elevation of B.P Presented by: Freya Cardozo 45
  • 46. Presented by: Freya Cardozo 46
  • 47. Presented by: Freya Cardozo 47
  • 48. Presented by: Freya Cardozo 48
  • 49. Presented by: Freya Cardozo 49 A solution containing 0.73 g of camphor (molar mass 152 gmol-1) in 36.8 g of acetone (boiling point 56.30C) boils at 56.55 0C. A solution of 0.564 g of unknown compound in the same weight of acetone boils at 56.46 0C. Calculate the molar mass of the unknown compound. [Oct 2014]
  • 50. Freezing point  Freezing of point of a liquid is the temperature at which the liquid and solid are in equilibrium and the two phases have the same vapour pressure Presented by: Freya Cardozo 50
  • 51. Depression in Freezing point  It is observed that addition of non volatile solute to solvent lowers the freezing point  Thus, The F.P of solution( with non-volatile solute)< F.P of pure solvent  Now, if Tf 0 is freezing point of pure solvent and Tf of the solution, Tf 0 > Tf  The difference between the two is called ∆ Tf Presented by: Freya Cardozo 51
  • 52. Freezing point depression & Vapour pressure lowering  Consider the vapour pressure diagram 1. Curve AB= V.P of solid solvent 2. Curve CD= V.P of pure liquid 3. Curve EF = V.P of solution  The vapour pressure of solution is always lower than the solvent and thus is present at the lower part of the graph  The non-volatile solute does not dissolve in the solid solvent Presented by: Freya Cardozo 52
  • 53.  Curve AB and CD  Intersect at B – This is where both the solid and liquid phases have the same V.P. Thus, The temperature corresponding to point B is freezing point of the pure solvent Tf 0  Curve EF and AB  Intersect at E – This is the point at which the solid solvent is in equilibrium with the solution Thus, The temperature corresponding to point E is freezing point of the solution Tf  It is clear from the figure that the freezing point of solution is lower than that of the pure solvent Presented by: Freya Cardozo 53
  • 54. But why so? DUE TO THE ATTRACTIVE FORCES BETWEEN THE MOLECULES  In pure liquid the attractive forces among molecules are large enough to cause the change of phase from liquid to solid  In solution, there are solute molecules in between the solvent particles.. this causes more separation of solvent molecules than in the solvent  Therefore, there is a decrease in the attractive forces between the solvent molecules. So the temperature of the solution is lowered below the freezing point of solvent to cause phase channge Presented by: Freya Cardozo 54
  • 55. Presented by: Freya Cardozo 55 Only solvent molecules Solute + solvent molecules Easier to change phase Solute molecules obstruct the phase change. More T needed(Lower Temps)
  • 56. Real life application Presented by: Freya Cardozo 56
  • 57. Freezing point depression and molality  Freezing point depression ∆Tf is directly proportional to molality of the solution  Kf= Freezing point depression constant / cryoscopic constant  If, m=1 ; ∆Tf = Kf  The cryoscopic constant thus is the depression in freezing point produced by 1 molal solution of a non volatile solute Presented by: Freya Cardozo 57
  • 58. Presented by: Freya Cardozo 58
  • 59. Relationship between Molar mass of solute and F.P depression Presented by: Freya Cardozo 59
  • 60. Presented by: Freya Cardozo 60
  • 61. Presented by: Freya Cardozo 61
  • 62. Osmosis  The net flow of solvent molecules into the solution through a semipermeable membrane OR  The net flow of solvent molecules into the solution from a more dilute solution to more concentrated solution through a semipermeable membrane is called osmosis Presented by: Freya Cardozo 62 SOLVENT SOLUTION Lower Conc. Higher conc.
  • 63. Semipermeable membrane  It is a film such as cellophane which has pores large enough to allow the solvent molecules to pass through them  The pores are small enough to not allow the flow of the larger solute molecules or ions of higher mass  Selectively allows passage of solvent molecules Presented by: Freya Cardozo 63 Solute molecules Semi- P.M Solvent molecules
  • 64. Osmotic pressure  In the thistle tube solution of interest (sugar solution) is placed and it is immersed in beaker filled with pure water  A semipermeable membrane is placed at the mouth of the tube  Some solvent passes through the membrane into the solution  This causes rise in liquid level in the tube  Now, the hydrostatic pressure in the tube pushes the solvent back into the container Presented by: Freya Cardozo 64
  • 65. Reverse osmosis  The liquid rises in tube and then stops, when the liquid stops rising that is the pressure which stops the flow and is called the osmotic pressure  This hydrostatic pressure that stops the osmosis is of the solution is the osmotic pressureΠ and is equal to 1. Height of the liquid column 2. Density of liquid column 3. acceleration due to gravity Presented by: Freya Cardozo 65
  • 66. Presented by: Freya Cardozo 66 Type Definition Examples Isotonic solutions Two or more solutions having the same osmotic pressure are said to be isotonic No net flow of solvent in either direction 0.1 M urea= 0.1 M sucrose Both have equal osmotic pressure but Different conc in g/L Hypertonic solutions If two solutions have unequal osmotic pressure, the more concentrated solution with the higher osmotic pressure is said to be hypertonic In a sucrose AND urea solution, Sucrose Higher osmotic pressureHypertonic Hypotonic solutions If two solutions have unequal osmotic pressure, the more dilute solution with the lower osmotic pressure is said to be hypertonic In a sucrose AND urea solution, Urea Lower osmotic pressureHyptonic
  • 67. Presented by: Freya Cardozo 67
  • 68. Osmotic pressure and conc. Of solution  For dilute solution the osmotic pressure can be given by,  V= volume of the solution in dm3 n2= number of moles of non volatile solute R= real gas constant = 0.08206 dm3 atm K-1 mol-1 Π= Osmotic pressure in atm Presented by: Freya Cardozo 68  We know that Concentration= n2/V  Concentration can be written in terms of Molarity M  Thus, equation becomes  Here, we can use molarity instead of molality because the osmotic pressures are measured at a constant temperature.
  • 69. Presented by: Freya Cardozo 69
  • 70. Molar mass of solute from osmotic pressure Presented by: Freya Cardozo 70
  • 71. Reverse osmosis  The direction of osmosis if from pure solvent to solution but this can be reversed by applying a pressure higher than the osmotic pressure  The pure solvent then flows from solution into pure solvent through semipermeable membrane. This is called reverse osmosis.  Eg. Fresh water and salty water separation using semipermeable membrane  On application of pressure higher than osmotic pressure, the salty water passes into fresh pure water  This leaves the salt behind Presented by: Freya Cardozo 71
  • 72. Presented by: Freya Cardozo 72
  • 73. Colligative properties of electrolytes 1. The solutions of electrolytes also exhibit colligative properties which do not obey the relations of non-electrolytes 2. The colligative properties of the solutions of electrolytes are greater than those to be expected for solutions of non electrolytes of the same concentrations 3. The molar masses of electrolytes in aqueous solutions determined by colligative properties are found to be considerably lower than the formula masses Presented by: Freya Cardozo 73
  • 74. Why is colligative properties of electrolytes more than nonelectrolytes Electrolytes- Dissociates Increases the number of particles Increase in colligative particles Eg. NaCl(lesser C.P) Vs Sucrose(more C.P) Presented by: Freya Cardozo 74
  • 75. Van’t Hoff factor (i)  In order to account for the dissociation/ association of electrolytes and to calculate their colligative properties Van’t Hoff suggested the factor i  It can be defined as the ratio of colligative property of a solution of electrolyte divided by the colligative property of nonelectrolyte solution of the same concentration.  No subscript  electrolyte solutions With subscript nonelectrolyte solutions Presented by: Freya Cardozo 75
  • 76. Definitions  It is also defined as , Presented by: Freya Cardozo 76 i=2 KNO3 NaCl i=3 CaCl2 Na2SO4 i=1 for non electrolytic solutions
  • 77. Why colligative properties of higher concentration solutions smaller than expected?  The electrostatic forces between the oppositely charged ions bring about the formation of ion pairs  Each ion pair consists of one or more cations and one or more anions held together by electrostatic attractive forces  This results in decrease in the number of particles in solution causing reduction in the expected I value and colligative properties Presented by: Freya Cardozo 77
  • 78. Modifications of expressions of colligative properties Presented by: Freya Cardozo 78
  • 79. Van’t Hoff factor i and degree of dissociation  For weak electrolytes Dissociation is related tαo Degree of dissociation α  Consider the equation  Initially 1 mol 0 0 At equilibrium (1- α)mol x α y α Total moles after dissociation = (1- α)+ x α + y α= 1+ α (x+y-1)= 1+ α(n-1) [Since, n=x+y] Vant Hoff factor can thus be given by, Presented by: Freya Cardozo 79
  • 80. Presented by: Freya Cardozo 80
  • 81. Presented by: Freya Cardozo 81
  • 82. Presented by: Freya Cardozo 82