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mole fraction, percentage (by volume and mass both), vapour pressure of solutions and Raoult’s Law - Ideal and non-ideal solutions, vapour pressure - composition, plots for ideal and non-ideal solutions; Colligative properties of dilute solutions - relative lowering of vapour pressure, depression of freezing point, elevation of boiling point and osmotic pressure; Determination of molecular mass using colligative properties; Abnormal value of molar mass,
van’t Hoff factor and its significance.
SOLUTIONS
A homogeneous mixture of two or more non-reacting substances is known as solution. Homogeneity or heterogeneity depends upon particle size and states of matter present in the solution. Every solution is made up of a solvent (present in larger quantity) and one or more solute (present in smaller quantity).
TYPES OF SOLUTION
Gaseous Solutions
Gas in gas
Liquid in gas
Solid in gas
Liquid Solutions
Gas in liquid
Liquid in liquid
Solid in liquid
Solid Solutions
Gas in solid
Liquid in solid
Solid in solid
CHAPTER INCLUDES
Types of solutions
Units of
concentration
Vapour pressure and Raoult's Law
Ideal and Non-ideal solution
Colligative properties
Lowering of
vapour pressure
Osmotic pressure
Elevation in boiling point
Depression in freezing point
Abnormal molecular mass and van’t Hoff factor(i)
UNITS OF CONCENTRATION
Molarity (M)
It is the no. of moles of solute present per litre of solution.
M × V
in cc =
W × 1000 M
mM = millimoles
Molarity changes with temperature of the solution. Increase in temperature decreases the molarity. It is the most convenient method to express concentration of the solution. On dilution molarity decreases.
Molality (m) :
No. of moles (n) of solute present per kg of solvent
It is independent of temperature since no volume factor is involved in the equation.
Mole fraction (x)
It is the ratio of no. of moles of one component to the total no. of moles present in the solution. For a system having two components A and B.
X = nA , X
= nB
nA + nB nA + nB
∴
Mole fraction is also independent of temperature.
In terms of %
% by weight =
wt.of solute wt.of solution
×100
% by volume
= wt.of solute vol.of solution
× 100 (In case of solid dissolved in a liquid)
% by volume =
volume of solute volume of solution
× 100
(In case of liquid dissolved in another liquid)
% by strength
= vol.of solute vol.of solution
× 100
% by weight is independent of temperature while % by vol., % by strength or strength are temperature dependent.
VAPOUR PRESSURE AND RAOULT’S LAW
The pressure exerted by the vapours at the free surface of liquid provided system is closed is known as its vapour pressure. The V.P. of a pure liquid is always greater than its solution (In case of non volatile solute).
Raoult’s Law for a solution having non volatile solute
⎡xsolute → molefraction of solute in solution⎤
⎢P° → V.P. of pure solvent ⎥
⎢⎣Ps → V.P. of solution ⎥⎦
i.e relative lowering of vapour pressure is equal to the mole fraction of solute.
Raoult’s Law of miscible liquid-liquid solution
For ideal solution the partial vapour pressure is directly proportional to their mole fraction at constant temperature. For two components A and B in liquid solution.
PA ∝ XA
⇒ PA
= P° XA
P°B
P°A
PB ∝ XB
⇒ PB = P° X
V.P
The total pressure P = PA + PB = P°A XA + P°B XB.
Most of the solutions show appreciable deviations from ideal behaviour known as real or non ideal solution. The characteristic property of these solutions is just the opposite to that of ideal solutions. In some cases the deviation is +ve while in some cases deviation is –ve.
IDEAL AND NON-IDEAL SOLUTIONS
The solutions which obey Raoult’s law are ideal solutions and those which do not obey Raoult’s law form non-deal solution.
Ideal Solution
Non-Ideal Solution
Positive Deviation
Negative Deviation
1. Obey’s Raoult’s law
1. Dis-obey’s Raoult’s law
1. Dis-obey’s Raoult’s law
2. pA = p°A.χA pB = p°B χB ptotal = pA + pB
2. pA ≠ p°A.χA pB ≠ p°B.χB
ptotal ≠ pA + pB [P > P + P ]
total A B
2. pA ≠ p°A.χA pB ≠ p°B.χB
ptotal ≠ pA + pB [P < P + P ]
total A B
3. ΔHmix = 0
ΔVmix = 0
3. ΔHmix = +ve
ΔVmix = +ve
3. ΔHmix = –ve
ΔVmix = –ve
4. Interaction
A – B ≈ A – A/B – B
e.g. Chlorobenzene + Bromobenzene
4. Interaction
A – B < A – A/B – B
e.g. CH3OH – H2O
4. Interaction
A – B > A – A/B – B
e.g. CH3COCH3 + CHCl3
p°A
p°B
p°A
p°B
p°A
p°B
χA = 1
χB = 0
χA = 0
χB = 1
χA = 1 χA = 0
χB = 0 χB = 1
χA = 1 χA = 0
χB = 0 χB = 1
COLLIGATIVE PROPERTIES
A colligative property of a solution is one that depends on the number of particle dissolved in it.
Relative lowering of vapour pressure,
Osmotic pressure, π = CRT.
Elevation of boiling point, ΔTb = kbm.
p° − ps
p°
= χsolute .
Depression in freezing point, ΔTb = kfm.
Relative lowering of V.P. : The relative lowering in V.P. of an ideal solution is equal to the mole fraction of solute at that temperature.
p° − p
n2 n2
w 2 M1
A A
pA
= χB =
n1 + n2
= n1
×
2 w1
Determination of molecular masses by relative lowering in vapour pressure.
p°−pA = w × M
p A m W
w = wt. of solute
m = Mol. wt. of solute W = wt. of solvent
M = Mol. wt. of solvent
Osmotic pressure : The excess pressure which must be applied on a solution to prevent the passage of solvent into it through a semipermeable membrane.
Determination : Barkley–Hartley method:
Semipermeable membrane → egg membrane;
Chemical Semipermeable membrane → cupric ferrocyanide.
π = CRT = n/V. RT; πV = nRT + van't Hoff equation for dilution solutions
n = w 2 ;
M2
M = w 2 .RT
2 πV B D
Elevation in boiling point: The property of rise in boiling point when some non volatile solute is added.
We know that the vapour pressure of the solution is lower than that of the pure solvent and vapour pressure increases with increase in temperature. Hence the solution has to be heated more to make the vapour pressure equal to the atmospheric pressure.
Alternatively, the elevation in boiling point may be explained on the bais of plots of vapour pressure versus temperature
Temperature
TO T
as follows :
Elevation in boiling point
Vapour pressure of the solvent increases with increase in temperature as shown by the curve AB. As at any temperature, vapour pressure of the solution is less than that of the solvent, the curve for the solution lies below that of the solvent, as shown by the curve CD. The temperatures at which the vapour pressure of the solvent and the solution become equal to the atmospheric pressure are T0 and T respectively. Obviously T > T0. The difference, called the elevation in boiling point, Δ Tb, is given by
Δ Tb = T – T0
Molal elevation constant or ebulioscopic constant, kb. It is the increase in boiling point when
the molality of the solution is unity.
ΔTb = kbm when m = 1, ΔTb = kb
WB × 1000 × k
MB =
ΔTb
WA
Depression in freezing point : The property of decrease in freezing point when some non-volatile solute is dissolved. The depression in freezing point is given by ΔTf
Freezing point : Temperature at which the liquid and the solid forms of the same substance are in equilibrium and hence have same vapour pressure.
We know that vapour pressure of the solution is less than that of the pure solvent. As freezing point is the temperature at which the vapour pressure of the liquid and the solid phase are equal, therefore for the solution, this will occur at lower temperature (lower the temperature lower the vapour pressure).
The graph explains this.
ΔTf = T°f – Tf
Tf Tf° Temperature
Molal depression constant. or cryoscopic constant (kf). It is the decrease in freezing point when the molality of solution is unity
ΔTf = kf.m
when m = 1, ΔTf = kf
M = WB × 1000 × k
B ΔTf × WA
Kb and Kf are intensive property of solvent and doesnot depend upon solute or solution.
ABNORMAL MOLECULAR MASS AND van’t HOFF FACTOR (i)
i = Experimental values of Colligative property Calculated value of colligative property
= Observedvalue of Colligative property Normal value of thesame property
= Normal moleculer mass = MC
Observed moleculer mass MO
Since Colligative property ∝ 1
molecular mass of solute
if i = 1, no molecular association or dissociation takes place if i < 1, molecular association takes place
if i > 1, molecular dissociation takes place.
For substances undergoing association or dissociation in the solution.
TEACHING CARE Online Live Classes https://www.teachingcare.com/ +91-9811000616
Relation between degree of association or dissociation (α) & van’t Hoff’s factor (i)
For association
where n = no. of particles that associate.
For dissociation
where n = no. of particles obtained on dissociation.
❑ ❑ ❑
PHYSICS-15-10- 11th (PQRS) SOLUTION
XI (PQRS) PHYSICS REVIEW TEST-5 Select the correct alternative. (Only one is correct) [15 × 3 = 45] There is NEGATIVE marking. 1 mark will be deducted for each wrong answer. Q.31 Two trains, which are moving along different tracks in opposite directions towards each other, are put on the same track due to a mistake. Their drivers, on noticing the mistake, start slowing down the trains when the trains are 300 m apart. Graphs given below show their velocities as function of time as the trains slow down. The separation between the trains when both have stopped, is: (A) 120 m (B) 280 m (C) 60 m (D*) 20 m 1 [Sol: x1 = 2 1 × 10 × 40 = 200 m; x2 = – 2 × 8 × 20 = –80 m xreletive = x1 + x2 = 280 separation = 300 – 280 = 20 m (D) ] Q.32 One end of a thin uniform rod of length L and mass M is riveted to the centre of a uniform circular disc of radius r and mass 2 M so that the rod is normal to the disc. The centre of mass of the combination from the centre of the disc is at dist
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