0% found this document useful (0 votes)
6 views3 pages

Solution

The document contains a series of chemistry exercises focused on vapor pressure, boiling point elevation, and colligative properties of solutions. It includes calculations related to the dissociation of solutes, mole fractions, and the effects of solute concentration on physical properties. The exercises also explore concepts such as ideal solutions and the behavior of volatile and non-volatile solutes.
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
0% found this document useful (0 votes)
6 views3 pages

Solution

The document contains a series of chemistry exercises focused on vapor pressure, boiling point elevation, and colligative properties of solutions. It includes calculations related to the dissociation of solutes, mole fractions, and the effects of solute concentration on physical properties. The exercises also explore concepts such as ideal solutions and the behavior of volatile and non-volatile solutes.
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
You are on page 1/ 3

Solutions Slot – 3 (Chemistry) Page # 19

EXERCISE – I SINGLE CORRECT (OBJECTIVE QUESTIONS)

7. AlCl3 = no. of particle = 4


1 1 CaCl2 = no. of particle = 3
1. y A  x A  
yA xA (vapour pressure of AlCl3) < (vapour pres-
sure of CaCl2 solution)
y A + yB x + xB TB.P. (AlCl3) > TB.P. (CaCl2)
< A T1 > T2
yA xA

y B xB y x 8. 100% dissociation
   A  A Tf = (0.0054) = i Kf m
yA xA y B xB = i × 1.86 × 0.001
=i=3
= 3 particles [MA6] A2
2. P  PA  PB  PA0  A  PB0  B
= 40 + 120 = 160 9. P = 0.95P0
PA = yA°P = yA × 160 Xsolvent = 0.95 , Xsolute = 0.005
 40 = yA × 160
 yA = ¼ P0  P n (Wsolute / M solute )
0
 
P N  n Wsolute  Wsolvent
P 0  P n solute n M solute M solvent
3.  
P n solvent N
M solute  M  M solvent  0.3M
P0  P n solute
(Wsolute / M )

P 0
nsolute  n solvent  0.05 
 Wsolute   Wsolvent 
 M  
   0.3M 
1 3 Wsolvent
4. xA  : xB    5.7
4 4 Wsolute
1 3 10. Pure A : XB = 0
PS   100   80  85
4 4 = PT = PA° = 120
1 Pure B : XB = 1
100  = PT = PB° = 120 - 75 = 45
PA 4  25  x1
yA   A
PS 85 85 11. (A) i = 1 + 0.90 (5 -1) = 1 + 3.6 = 4.6
(B) i = 1 + 0.90 (3 -1) = 2.8
60 (C) i = 1 + 0.9 (3 -1) = 2.8
yB   x1B (D) i = 2.8
85 Ans : (A) Higher the value of i means Boiling
25 0 point will be higher.
Pdistilate =  100   80
85 85
= 85.88 mm Hg 0
12. P  P
 X solute
5. less no of particle of solute means maximum P0
vapour pressure. P 0  P  X solute
6. Glucose does not dissociate 10 0.2

i=1 20 X solute
 X solute  0.4  X solvent  0.6
Page # 20 Solutions Slot – 3 (Chemistry)

13. M = 1 d = 1.2 Mol mass = 180 17. PT = 200XA + 100XB

1000  M XA = XB = ½ (given)
m=
1000d  M  180  PT = 150
If all the liquid become vapour then PT can be
1000 1000 calculated by
 
1200  180 1020
1 1  1 1
1000   yA  0  0 
Tb  K b  0.98 K b PT PB0  PA PB 
1020
 PT  133.3

actual mole of solute(Experiment)


14. i = theoritical mole of solute then pressure at which half of liquid converted
into vapour must be in the range of
MT 133.3 < P < 150
i
Mexp.
2 3
18. P = 100 × + 300 ×
i = 1 +  (n - 1) = 1 +  (3 - 1) 5 5

 i  1  2  i  1 = 40 + 180 = 220
M
 T 1
Mexp 19. For ideal solution

 MT  Mexp Hmix  0
 Mexp  111 Gmix  0
Smix  0

15. i = 1 +  (5 - 1)
= 1 + 0.6(4) = 3.4
20. Only solvent molecules can go through SPM,
Tb = 3.4 × 0.52 × 1 not the solute particles hence no blue colour
= 1.768 formation

Tb1 = 373 + 1.768

= 374.76 P0  P 1000
22.  m
P Msolvent

1 1  1 1
16. P  P0  y A  P0  P0  17.25  17.20 1000
B  A B  m   0.1615
17.20 18

1/Pº
If m = M = 0.1615
B

XCl3 
 X  3Cl

1/P 1/Pº
A
Mtotal = S + 3S = 4S = 0.1615
S = 0.040375
yA=0 yA=1
= 4.037 × 10–2
Solutions Slot – 3 (Chemistry) Page # 21

23. Initially A = 3 mole ; B = 2 mole


 1.38  10 3

3 0 2 0 26. i = 1 + (n  1)
600 = P  P ...... 1
5 A 5 B
2.74 = 1 + (3  1)
finally A= 4.5 mole ; B = 2 mole and c = 0.5
mole    0.87

 Degree of dissociation = 87%


4.5 0 2 0
630 = P  P
7 A 7 B
27. 1.04 = 0.52 × m  m = 2
PA0 = 940
P0  750 1000
0
2 
P  90
B 750 18

 P0 = 777 = Patm
24. B.PTolulene > B.P.Benzene P0 = Patm (because at T water boils)
V.P.Tolene < V.P.Benzene So at T : P0 = Patm
Benzene is more volatile (By graph) because when water boils V.P. become equals
xBenzene < yBenzene to atmospheric pressure

(A) If xB = 0.5  yt = 0.2, yB = 0.8


(B) xt = 0.3,  xB = 0.7  yB = 0.6 not pos- 28. Freezing is exothermic because to freeze wa-
sible ter Heat must be removed.

(C) xB = 0.3 and yt = 0.4 1> False

 yB = 0.6 correct 2> True.

(D) xB = 0.7. yB > 0.7 (should be)


Given yt < 0.3  yB > 0.7 correct 29. Addition of non-volatile will decrease the
freesing point and in case of addition of vola-
tile substance then it is not necessary Hence
25. 0.20 = 1.8 × M × i
Statement 1 True
0.20 20 10 Hx
i   H x
 
Statement 2 False
0.1 1.8 18 9 0.1 0.1 0.1 0.1

10
i= and i = 1 +  (2-1) = 1 + 
9

1

9

 1
 0.1 
2
0.1  81 
K 
1  1
1
9

You might also like