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SOLUTIONS
BY
DR. LALIT KUMAR SHARMA
Associate Professor
Advanced Educational Institutions
Aurangabad(Palwal)
www.advanced.edu.in
Solution
A solution is a homogeneous mixture of two (or more) substances, the composition of which may
vary between certain limits. A solution consisting of two components is called binary solution. The
component which is present in large quantity is called solvent and the component which is small in
quantity is called solute. If both components are in same physical state.
Type of Solutions: The three states of matter (gas, liquid or solid) may behave
either as solvent or solute. Depending on the state of solute or solvent, mainly
there may be the following seven types of binary solutions.
S.No. Solute Solvent Example
1 Gas Gas Air
2 Gas Liquid Aerated water (CO2 + H2O)
3 Gas Solid Hydrogen in palladium
4 Liquid Liquid Alcohol in water, benzene in toluene
5 Liquid Solid Mercury in zinc amalgam
6 Liquid Gas CO2 dissolved in water
7 Solid Liquid Sugar in water, common salt in water
8 Solid Gas Smoke
9 Solid Solid Various alloys
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Vapour Pressure:
 The pressure exerted by vapours over the liquid surface at equilibrium is called vapour pressure of
the liquid.
 If solute is non volatile solid or liquid the vapour pressure of solution is equal to partial vapour
pressure of solvent in the solution.
 If the solute is volatile solid or liquid, then vapour pressure will be equal to the sum of partial vapour
pressure of solute and that of solvent.
Raoult’s Law:
“The partial vapour pressure of any component in the solution is directly proportional to its mole
fraction”.
 For a binary solution of two components A and B,
PA = XA and PB = XB
Where
P0
A = vapour pressure of component A in pure state.
PA = vapour pressure of component A in the solution.
P0
B = vapour pressure of component B in pure state.
PB = vapour pressure of component B in the solution
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Limitations of Raoult’s Law :
 Raoult’s law is applicable only to very dilute solutions.
 It is applicable to solutions containing non-volatile solute only.
 It is not applicable to solutes which dissociate or associate in a particular solution
Raoult’s Law in Combination with Dalton’s Law of Partial Pressure:
PT = XA P0
A + XB P0
B = P0
B + (P0
A -P0
B) XA Where PT = Total Vapour Pressure of the Solution.
Ideal and Non-Ideal Solutions:
 Ideal Solution: These solutions obey Raoult’s law at all compositions of solute in solvent at all
temperature . Two liquids A and B form and ideal solution when A –A and B–B molecular attractions
will be same and hence A–B molecular attraction will be almost same as A–A and B–B molecular
attraction.
For Ideal Solution:
1. dHmixing = 0, i.e. no heat should be absorbed or evolved during mixing
2. dVmixing = 0, i.e. no expansion or contraction on mixing
Examples , Ethyl chloride and ethyl bromide, n–hexane and n–heptane , CCl4 and SiCl4
www.advanced.edu.in
 These solutions deviate from ideal behaviour and do not obey Raoult’s law over entire range of
composition.
For non ideal solutions,
1. dHmixing ≠ 0 2 dHmixing ≠ 0
Here we may have two cases
A) Positive Deviation:
1. PA > XA & PB > XB
2. dHmix > 0
3. dVmix > 0
Example: Cyclohexane and Ethanol
B) Negative Deviation:
1. PA > XA & PB > XB
2. dHmix < 0
3. dVmix < 0
www.advanced.edu.in
Non-Ideal Solution:
Colligative Properties :
The properties of dilute solutions which depend only on number particles of solute present in
the solution and not on their identity are called colligative properties (denoting depending
upon collection).
Lowering of Vapour Pressure by a Non-Volatile Solute
The relative lowering of vapour pressure of a solution containing a non-volatile solute is equal to the
mole fraction of the solute present in the solution.
Elevation of Boiling Point by a Non-Volatile Solute :
Since the addition of a non-volatile solute lowers the vapour
pressure of the solvent, the vapour pressure of a solution
is always lower than that of the pure solvent, and hence it must
be heated to a higher temperature to make its vapour pressure
equal to atmospheric pressure.
where M1 = molecular weight of solute and w2 and w1 are weights of solute and solvent
www.advanced.edu.in
where M1 = molecular weight of solute and w2 and w1
are weights of solute and solvent
Osmosis: The phenomenon of the passage of pure solvent from a region of lower concentration (of the
solution) to a region of its higher concentration through a semi-permeable membrane.
Osmotic Pressure: Excess pressure which must be applied to a solution in order to prevent flow of solvent into
the solution through the semi-permeable membrane.
V = nRT
= Osmotic pressure
V = volume of solution
n = no. of moles of solute that is dissolved
R = Gas constant
T = Absolute temperature
Isotonic Solutions: A pair of solutions having same osmotic pressure is called isotonic solutions.
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Depression of Freezing Point by a Non-Volatile Solute:
 Van't Hoff Factor: Van't Hoff, in order to account for all abnormal cases introduced a factor i known
as the Van't Hoff factor, such that
 Degree of Association: The fraction of the total number of molecules which combine to form
bigger molecule
Let a be the degree of association, then,
The number of unassociated moles = 1-
The number of associated moles = /n
Total number of effective moles = 1 - + /n
Obviously, i < 1
www.advanced.edu.in
Abnormal Molecular Weight and Van't Hoff Factor:
Degree of Dissociation :
 The fraction of the total number of molecules which dissociates in the solution, that is, breaks into
simpler molecules or ions.
KCl ↔ K+ + Cl-
1 -
Thus, the total number of moles after dissociation = 1 - + + = 1+
Hence, i = (1+ )/1
i = 1+ = 1+ (2–1)
In general, i = 1+ (n–1) ,
Where, n = number of particles ( ions) formed after dissociation
From the above formula, it is clear that i > 1
www.advanced.edu.in
Thank you
DR. LALIT KUMAR SHARMA
Associate Professor
Advanced Educational Institutions,
70 km Milestone,
Delhi-Mathura Road, Dist. Palwal, Haryana-121105
+91–1275–398400, 302222
lkspwl76@gmail.com
www.advanced.edu.in

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Solution

  • 1. SOLUTIONS BY DR. LALIT KUMAR SHARMA Associate Professor Advanced Educational Institutions Aurangabad(Palwal) www.advanced.edu.in
  • 2. Solution A solution is a homogeneous mixture of two (or more) substances, the composition of which may vary between certain limits. A solution consisting of two components is called binary solution. The component which is present in large quantity is called solvent and the component which is small in quantity is called solute. If both components are in same physical state. Type of Solutions: The three states of matter (gas, liquid or solid) may behave either as solvent or solute. Depending on the state of solute or solvent, mainly there may be the following seven types of binary solutions. S.No. Solute Solvent Example 1 Gas Gas Air 2 Gas Liquid Aerated water (CO2 + H2O) 3 Gas Solid Hydrogen in palladium 4 Liquid Liquid Alcohol in water, benzene in toluene 5 Liquid Solid Mercury in zinc amalgam 6 Liquid Gas CO2 dissolved in water 7 Solid Liquid Sugar in water, common salt in water 8 Solid Gas Smoke 9 Solid Solid Various alloys www.advanced.edu.in
  • 3. Vapour Pressure:  The pressure exerted by vapours over the liquid surface at equilibrium is called vapour pressure of the liquid.  If solute is non volatile solid or liquid the vapour pressure of solution is equal to partial vapour pressure of solvent in the solution.  If the solute is volatile solid or liquid, then vapour pressure will be equal to the sum of partial vapour pressure of solute and that of solvent. Raoult’s Law: “The partial vapour pressure of any component in the solution is directly proportional to its mole fraction”.  For a binary solution of two components A and B, PA = XA and PB = XB Where P0 A = vapour pressure of component A in pure state. PA = vapour pressure of component A in the solution. P0 B = vapour pressure of component B in pure state. PB = vapour pressure of component B in the solution www.advanced.edu.in
  • 4. Limitations of Raoult’s Law :  Raoult’s law is applicable only to very dilute solutions.  It is applicable to solutions containing non-volatile solute only.  It is not applicable to solutes which dissociate or associate in a particular solution Raoult’s Law in Combination with Dalton’s Law of Partial Pressure: PT = XA P0 A + XB P0 B = P0 B + (P0 A -P0 B) XA Where PT = Total Vapour Pressure of the Solution. Ideal and Non-Ideal Solutions:  Ideal Solution: These solutions obey Raoult’s law at all compositions of solute in solvent at all temperature . Two liquids A and B form and ideal solution when A –A and B–B molecular attractions will be same and hence A–B molecular attraction will be almost same as A–A and B–B molecular attraction. For Ideal Solution: 1. dHmixing = 0, i.e. no heat should be absorbed or evolved during mixing 2. dVmixing = 0, i.e. no expansion or contraction on mixing Examples , Ethyl chloride and ethyl bromide, n–hexane and n–heptane , CCl4 and SiCl4 www.advanced.edu.in
  • 5.  These solutions deviate from ideal behaviour and do not obey Raoult’s law over entire range of composition. For non ideal solutions, 1. dHmixing ≠ 0 2 dHmixing ≠ 0 Here we may have two cases A) Positive Deviation: 1. PA > XA & PB > XB 2. dHmix > 0 3. dVmix > 0 Example: Cyclohexane and Ethanol B) Negative Deviation: 1. PA > XA & PB > XB 2. dHmix < 0 3. dVmix < 0 www.advanced.edu.in Non-Ideal Solution:
  • 6. Colligative Properties : The properties of dilute solutions which depend only on number particles of solute present in the solution and not on their identity are called colligative properties (denoting depending upon collection). Lowering of Vapour Pressure by a Non-Volatile Solute The relative lowering of vapour pressure of a solution containing a non-volatile solute is equal to the mole fraction of the solute present in the solution. Elevation of Boiling Point by a Non-Volatile Solute : Since the addition of a non-volatile solute lowers the vapour pressure of the solvent, the vapour pressure of a solution is always lower than that of the pure solvent, and hence it must be heated to a higher temperature to make its vapour pressure equal to atmospheric pressure. where M1 = molecular weight of solute and w2 and w1 are weights of solute and solvent www.advanced.edu.in
  • 7. where M1 = molecular weight of solute and w2 and w1 are weights of solute and solvent Osmosis: The phenomenon of the passage of pure solvent from a region of lower concentration (of the solution) to a region of its higher concentration through a semi-permeable membrane. Osmotic Pressure: Excess pressure which must be applied to a solution in order to prevent flow of solvent into the solution through the semi-permeable membrane. V = nRT = Osmotic pressure V = volume of solution n = no. of moles of solute that is dissolved R = Gas constant T = Absolute temperature Isotonic Solutions: A pair of solutions having same osmotic pressure is called isotonic solutions. www.advanced.edu.in Depression of Freezing Point by a Non-Volatile Solute:
  • 8.  Van't Hoff Factor: Van't Hoff, in order to account for all abnormal cases introduced a factor i known as the Van't Hoff factor, such that  Degree of Association: The fraction of the total number of molecules which combine to form bigger molecule Let a be the degree of association, then, The number of unassociated moles = 1- The number of associated moles = /n Total number of effective moles = 1 - + /n Obviously, i < 1 www.advanced.edu.in Abnormal Molecular Weight and Van't Hoff Factor:
  • 9. Degree of Dissociation :  The fraction of the total number of molecules which dissociates in the solution, that is, breaks into simpler molecules or ions. KCl ↔ K+ + Cl- 1 - Thus, the total number of moles after dissociation = 1 - + + = 1+ Hence, i = (1+ )/1 i = 1+ = 1+ (2–1) In general, i = 1+ (n–1) , Where, n = number of particles ( ions) formed after dissociation From the above formula, it is clear that i > 1 www.advanced.edu.in
  • 10. Thank you DR. LALIT KUMAR SHARMA Associate Professor Advanced Educational Institutions, 70 km Milestone, Delhi-Mathura Road, Dist. Palwal, Haryana-121105 +91–1275–398400, 302222 lkspwl76@gmail.com www.advanced.edu.in