xii class jee shikhar solution 20-12-2015
TRANSCRIPT
8/17/2019 Xii Class Jee Shikhar Solution 20-12-2015
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JEE TEST SERIES / PART TEST # 03 / PAPER – 1 & 2 / SOLUTION / PAGE - 1
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JEE TEST SERIES PART TEST # 03
(XII + DRP) PAPER – 1 (ADVANCED) SOLUTIONS
PART I : PHYSICS
SECTION – 1 : (One Integer Value Correct Type)
Sol.1. (B) N = mg 2N mr
2mg m.2sin g
2sin
0.1 10
2 sin30
1rad / s.
Sol.2. (AC)
Sol.3. (C) B must be appearing at infinity
2 1 2 1h
2R
Solving 1
2
2
Sol.4. (AC) P = 0.5 W Energy delivered in 5 sec
E P t E 0.5 5 2.5J
This E will be in form of KE21
E mv2
212.5 0.2 v
2 v 5m / s
Sol.5. (BC) For pure rolling
2 R 5 R 7 3 7 73
X '7'
Sol.6. (AC) A ' 30t,100 2 40t B' 10t, 0
222
A 'B' 10t 30t 100 2 40t 0
222s 40t 100 2 40t
sds
2 2 40t .40 2 100 2 40t . 40
dt
For min
dss 0
dt
Solving this
20 5t 2 2
16 4
X 2
4
5 2
4 X '5'
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60°
O
60°
B
A C
B
A
C
90 + r
20
)(2
r
310
y
A
D x
B
v t 0
Sol.7. (C) Using law of sine in ABC
10 3
sin=
20
sin(90 ) cos( )
AC
r r
... (i)
Snell’s law, 1 × sin 60 =3
sin2
r ... (ii)
AC = 4.1 cm
–102.07 10'
AC t
C s
Sol.8. (BD) 00 sin
v t x v t r
r
0cosv t
y r r r
Differentiating above equations
00 1 cos x
v t v v
r
00 siny
v t v v
r
2 2 002 sin
2 x y
v t v v v v
r
SECTION – 2 : (One or More Than One Option Correct Type)
Sol.9. (AC) Impulse = Change in momentum
= 2 12 v v ˆ ˆ2 3i j
As impulse is in the normal directing of colliding surface1
tan3
1 1tan
3
0 1 1
90 tan3
Sol.10. (ABC) v a
Sol.11. (BD)
Sol.12. (AC)
Sol.13. (ABCD) Maximum elongation =2F
k and equilibrium is at
F x
k
Amplitude =2F F F
k k k
Sol.14. (ABC) By Center of Linear Momentum
9 4 3 8 4 1 8V
2 /V m s
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2 1 3 1
9 3 12 4e
2 21 1
4 1 8 2 182 2
f E
2 21 1
4 9 8 3 198
2 2
i E
loss = 18 198 180f i E E J
Sol.15. (ABD) 2 2v ax bx c (equation for parabola)
On differentiating
2 2vdv
ax bdx
2
vdv bax
dx
acceleration
0
at2
b x
a
Which is the vertex of parabola2 x x
After1 x velocity is increasing, hence v and a are in same direction.
After2 x velocity is decreasing, hence v and a are in opposite direction.
Sol.16. (AB) If x = a sin (t + )
Then V =dx
dt
= a cos (t + )
a =dv
dt = – a
2sin (t + )
Time period, T = const.
(B)aT
x = –
2T = const.
(A) a2T
2 + 4
2v
2= a
2
4 sin
2(t + ).
2
2
4
+ 4
2a
2
2 cos
2 (t + )
= a2
2 4
2[sin
2(t + ) + cos
2(t + )]
= a2
24
2= const.
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Sol.17. (ABC) The path difference at C is = t ( – 1)
It may or may not be equal to n. Hence maxima may or may not occur at C .
(i) If t ( – 1) = n, the maxima will occur at C .
(ii) If ( 1) (2 1)2
t n
, the minima will occur at C .
(iii) The position on the screen where path difference = 0 is called central maximum
position.
(iv) The intensity at the point of minima will be zero only when 1 2I I .
Here I 1 I 2
At the minima, intensity will not be completely zero.
Hence (C) is the incorrect option.
Sol.18. (ACD) Use Snell’s law
SECTION – 3 : (Matrix Match Type)
Sol.19. (B) (P) The body is in pure rolling & there is no external force on it hence there is no friction(A), (B), (C), (D).
(Q) There is no torque about P and collision is elastic.
(B), (C), (D)
(R) There is no torque about P and collision is inelastic.
(B)
(S) Force acting is Mg (conservative). It will have a torque about P.
(T) Gravitational force is conservative, the force between these particles is internal force.
(A), (C), (B).
Sol.20. (C) For no emergence
c A 2 c
A / 2 c1sin
A 1sin2
2
For no emergence
c c A c csin A sin c
1sin A
csin A 1
Total internal reflection at 2x
2 cminr
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PART II : CHEMISTRY
SECTION – 1 : (One Integer Value Correct Type)
Sol.21. (AB) 2NO + O2 2NO2
(moles before reaction) 1 0.5 0
after reaction 1 –.5 0.5 1
= 1.5
n = |1.5 – 2.5| = 1
Change in pressure
P =nRT
V
=1 ×
1
12×
300
6.25 atm = 4 atm
Sol.22. (BD) Balanced equation is –
3I2(s) + 6 OH – 5I
– + –
3IO + 3H2O()
G° = 5×( –50) + ( – 123.5) + 3×( –233)
–0 – 6 × ( –150) = – 172.5 KJ/mol
Now
G° = – RTnk
– 172.5 =25
–
3 × 300 × 2.3 × 10
–3 log K
log K = 30
1030
= – 5 – –5 –1
3
– 6 – 6
[I ] [IO ] 10 10
[OH ] [OH ]
[OH –] = 10
–6
pOH = 6
pH = 8
Sol.23. (B) 2eq. of K2Cr 2O7 and eq. of SO2 = 1 mol of SO2
2SO2(g) + O2(g) 2 SO3(g)
1 mol 1 mol 0 mol
1 mol 0.5 mol 1 mol
2SO 1P
2.5 × 5 = 2 Atm,
2O
0.5 5P
2.5
= 1 Atm
3SO
1P
2.5 × 5 = 2Atm
Kp =
3
2
22
SO
2 2
SO
P 21.0
P 2 1
Sol.24. (AC) AB2(g) AB(g) + B(g)
Initial 100 0 0
At equ. 100 – x x x At eq. P = 120
120 = 100 – x + x + x
= 100 + x = 120x = 20
Kp =x x 20 20
100 – x 100 – 20
= 5
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Sol.25. (C)
Initially :
At equilibrium :
CH3COOH + C2H5OHK C
CH3 COO C2H5 + H2O
0.1 mol 0.1 mol 0 0
(0.1 – x) mol (0.1 – x) mol x x
In 10 ml solution at equilibrium moles of
CH3COOH present = 0.1 (0.1 – x) 0.1 (0.1 – x)
moles of NaOH 0.1 (0.1 – x) = 80 × 10
–4 = 8 × 10
–3
or 0.01 – 0.1 x = 0.008
or x = 0.02
KC =2 2
2 2 2
x (0.02) 1 1
16(0.1 – x) (0.08) 4
= 32 KC = 32 ×1
16 = 2
Sol.26. (AC)
Sol.27. (C) Anhydride formation
Sol.28. (AC) W A B = – 10 J
W AB = PV ; WBC = 0
q = E – W
E = 0
q = 5 = 0 – W
W = – 5J = W A B + WB C + W C A
or – 5 J = – 10 + 0 + WC A
WC A = 5 J
SECTION – 2 : (One or More Than One Option Correct Type)
Sol.29. (BC) Sol.30. (C) Sol.31. (AD) Sol.32. (BC)
Sol.33. (AD) Sol.34. (AD) Sol.35. (AC) Sol.36. (BC)
Sol.37. (AB) Sol.38. (ABC)SECTION – 3 : (Matrix Match Type)
Sol.39. (D) Sol.40. (C)
SECTION – 1 : (One Integer Value Correct Type)
Sol.41. (D) f x x 1 x 2 x 3 x 4
2 2x 5x 4 x 5x 6
Now let 2x 5x t and t t 4 t 6
2t 10t 24
min
t 1 for t 5
and 2x 5x 5 has real roots
M 1 M 4 3.
PART III : MATHEMATICS
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Sol.42. (C) 2 2 2 3
2 2
dy dx 1 1x y x y dy 0
y xy x
1 1d
x y1 1 1 1d y dy 0 ydy
1 1x y y x
x y
21 1 yln c k 2.
x y 2
Sol.43. (A) sinxcosy f 2x 2y f 2x 2y cosx.siny f 2x 2y f 2x 2y
f 2x 2y sin x y
f 2x 2y sin x y
f f k
sin sin2 2
x
f x k sin 2
4f ' x f x 0.
Sol.44. (AD) Since 2 x xsin cos
4 4 lies between 1 and 2 for x 2, 2
2 x xsin cos 1
4 4
Thus the problem reduces to finding the area bounded by 2 2 2x y 4, y x x 1 and line
y = 1
Now required area 2 0
2 2
13
2 3 2 4 x dx 1 x x 1 dx
2 13 k 6.
3 6
Sol.45. (D) /2
/2
1 2f x sinx sinx tcosx sint cost dt
k k
1 2 3 4sinx l l l l
Where,/2
1
/2
sinxl sin tdt 0
k
/2
2
/2
2sinx 4sinxl costdtk k
/2
3
/2
cosx 2cosxl t sin tdt
k k
/2
4
/2
2cosxl tcostdt 0
k
t cost is odd
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1 2 4sinx 2cosx
sinx cosx sinxk k k k
1 41 k 3.
k k
Sol.46. (D) 1 1f x tan tan x cos cos x for3
x ,2 2
when x x x 02 2 2
x 02
tan x tan x tanx
1 1f x tan tanx cos cosx x x 2x
When 3 3
x x x 0 x2 2 2
0 x2
and x 2 x2
and cos 2 x cos x
f x x 2 x
So graph of f(x) and required area is shown in figure
2 22 3
area .4 4
Sol.47. (B) tanx 0, tanx 1
3
3 3
3
33
log 3 log 3
log tanx 1log tanxlog 3
Let3
log tanx 1 0
2t 3 1
t 2 2
t 3 1t
23t 2t 1 0
t 1 and1
t3
(not possible)
3log tan x 1
1
tanx x 63
only in 0, .
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Sol.48. (B)
2 x 12
2
x e , 0 x 1f x a b 1
acos 2x 2 bx , 1 x 2
2 x 1 2 x 122xe 2x e , 0 x 1f ' x b 2
2bx 2asin 2x 2 , 1 x 2
SECTION – 2 : (One or More Than One Option Correct Type)
Sol.49. (ACD) Let f ' x 0
1 1 1 1 3 3f , f , f
2 2 4 4 4 4
and so on
f x x
Let f ' x 0
1 1 1 3 3 1
f , f , f 2 2 4 4 4 4
And so on
f x 1 x
Sol.50. (AD) sinx cosx
sin x cos xe cos x e sinxf ' x e e
cosx sinx
f g x x f ' g x g' x 1
1g' x
f ' g x
1/ 21 1 eg' 0
5 2f ' g 0f '
4
Sol.51. (BC) Given curve is3 2 23 12 3 6 12
dy dy y x y y x
dx dx
23 4 6dy
y x dx
2
2
42
24
y dy x dx
dx dy x y
Here, 0dx
dy
2 40 2
2
y y
x
But 2y gives 2 28 3 24 3 16 x x
2 2 162 3 12 2 8 16
3
y x x
Required point is4
, 23
Sol.52. (AD) 4 3 3 2 4 3 21 4 3 4 2 3 4 A x x Bx C x x x x x
4, 2, 1 A B C
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3 2
3/ 24 3 4 3
2 1 4 34
1 1
x x x dx f x
x x x x
1/2 1/2 1/24 3 4 3 4 3 4 3
2 2 1 2 2 144
1 1 1 1
x x dx dx c
x x x x x x x x
f 1 6
Sol.53. (AB) 2x
2 2
0
f x f t1 dt
1 x 1 t
2 2
2 22
1 x f ' x 2xf x f x
1 x1 x
2
2
dy 2xy y
dx 1 x
Let1
ty
2
dt 2xt 1
dx 1 x
solution is 3
21 x1 x x c
y 3
But 2
3
3 1 xf 0 1 c 1 y f x
x 3x 3
f 1 6
Sol.54. (ABC) The graph of g(x)
Sol.55. (BD) Area =
3 32 2 26 5 4 3 2
1 1x ax bx cx dx ex f mx n dx x 1 x 2 x 3 dx
1 1 1
22 22 2 2 2 4 2
1 1 0
t t 1 t 1 dt t t 1 dt 2 t t 1 2t dt
= 1 1 2 15 35 42 16
2 27 3 5 105 105
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Sol.56. (AD) We have 2y x 2 2y 2 xf x 2y f x e f 2y e x 1 e 4y 1 e 4xy
Putting x y 0, we get f 0 2f 0 f 0 0
Now
y 0
f x 2y f xf ' x lim
2y
2y x 2 2y 2 x
y 0
f x e e f 2y x 1 e 4y 1 e 4xy f xf ' x lim
2y
2y 2y
x 2
y 0 y 0 y 0
e 1 e 1f 2y f 0f ' x f x lim e lim x lim 2x
2y 2y 2y
x 2f ' x f x e f ' 0 x 2x
x x x 2 xe f ' x e f x f ' 0 2xe x e
x x x 2 xe f ' x e f x 1 2xe x e
x 2 xd de f x x x e
dx dx
x 2 xe f x x x e c f 0 0 c 0
x 2f x xe x g x x and xh x e .
Sol.57. (AC) Equality is true if f(t) g(h(t)) = f(h(t)) g(t) or f(t).g(h(t)) = f(h(a + b – t)) g(a + b – t)
Sol.58. (ABC) Hence,
x 3 2 x 2 x 1 , x 3
x 3 2 x 2 x 1 , 3 x 2f x
x 3 2 x 2 x 1 , 2 x 1
x 3 2 x 2 x 1 , x 1
i.e.
2, x 3
2x 8, 3 x 2
f x 2x, 2 x 1
2, x 1
maxf 4 at x 2 and minf 2 at x 1 2f x m 3m will have no solution if
2m 3m 4 or 2
i.e. if 2m 3m 4 0 or 2m 3m 2 0 i.e. if m 4 m 1 0 or m 2 m 1 0
i.e. if m 4 or m 1 or 2 m 1
SECTION –
3 : (Matrix Match Type)Sol.59. (C) (A) Let x = sinθ and y = cosθ
x y sin cos
2sin4
minimum value = 2 .
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(B)1
y acosx cos3x3
y ' 06
asin sin 06 2
a 2.
(C) f ' x 1 2 cos x 1
f ' x 0 cosx2
5x ,
3 3
a b 2.
(D) At x 0, y 1 also 1
y ' 02
equation of tangent 1
y 1 x 02
x y1 p q 3.
2 1
Sol.60. (B) (A) 2 3 21 sin x 24 sin x cosec x cosecx 24 cosec x 3
(B) 2 2f ' x 6x 2bx 4 cos x
f ' x 0 x R
2 26x 2bx 4 cos x 0 x R
26x 2bx 4 0 x R
23x bx 2 0 2b 24 0
24 b 24 b 0, 1, 2, 3, 4
(C) If 1 1sin sinx cos cosx , then 0 / 2.
Consider 4 different cases.
1
2
3
4
C 1 sinx 0
C 0 sinx 1
C sinx 0
C sinx 1
The solution set is 2n , 2n , n z2
(D) Let
2x
2xL lim 1 ,
x x
it is of form 1
2
22x 1 1 2
2x xx
x xL lim e lim e e
1
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JEE TEST SERIES PART TEST # 03
(XII + DRP) PAPER – 2 (ADVANCED) SOLUTIONS
PART I : PHYSICS
SECTION – 1 : (One Integer Value Correct Type)
Sol.1. (AC)
2
1 2
2
1 2
I I 49
9I I
Solve we get
1
2
I 5
2I 1
2
I 25
I 4
25I
4
4 4 25I 5
5 5 4
Sol.2. (AC)
Sol.3. (AB) T mg cos 2
P oscI w mgx 2
2
osc
mlw mgR
12
cos 1
For small and x R for small
osc 2
12gRw
l
2 2 l lT
w 12gR 3gR
T
3
12 12T 4
3
Sol.4. (AC)
Sol.5. (BD) Image is real
v
7u
7
77 u
1 7 u
1 7 u
u 8
Sol.6. (B) This would happen if there is no collision with the wall
on reaching RS = 0
2 21 1kx mv
2 2
2
21100 1 v
100
v 1/ ms
Sol.7. (AC) Particle is released at x 2
max at
min.u i f
TE TE 2110 15 mv
2
125
2 2 2
5 m / s Sol.8. (B) First reflection from (1) then
1 1 1
V 15 10
v 30
x
mg
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1
30m
15
Next reflection from (2) from
1 1 1
v ' 10 10
v ' 5
2
5m
10
Total magnification
1 2m m m
30 5
15 10
m 1
Image is real & inverted.
SECTION – 2 : (One or More Than One Option Correct Type)
Sol.9. (CD)
2
x Asinwt
v Awcoswt
a Aw sin wt
2 2 2 2v A w cos wt
22
2 2
vcos wt
A w …… (1)
2 2 4 2a A w sin wt
22
2 4
asin wt
A w ……. (2)
Add equation (1) and (2)2 2
2 2 2 4
v a1
A w A w
(A) 2v y a x
2
2 2 2 4
y x1
A w A w (Parabola)
(B) 2v y 2a x
2 2 2 4
y x1
A w A w (Straight line)
(C) v y a x
2 2
2 2 2 4
y x1
A w A w (Ellipse)
(D) v y 2a x
2
2 2 2 4
y x1
A w A w (Parabola)
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Sol.10. (D)
Sol.11. (BCD)zF n mg 20 0 N mg 20 N 50 20 N 30
maxf N
0.4 30
12
Eternal force in the plane of surface =ˆ ˆ
6i 8 j =10 Nf 10N
F will be opposite to external force
Contact force
2 2
2 2
N f
30 10
10 10
Sol.12. (ABC)1 1 1
f v u
1 1 1
v f u f constant
1 1
kv u
1 1
versusv u is linear 1 1 1
f v u u u
1f v
u u1
v f
uku 1
v straight line.
Sol.13. (ABC) There is no external force acting on the system
a 0 p 0
constant
Sol.14. (BD)
Sol.15. (ABD) T 40N 2a 10 m / s KE 40J 21mv 40
2
1
22 2v 40 2v 40
2 2v a 2as 40 0 2 10 s
s 2m
mgW Mg h
2 10 2
40 J
TW 40 2
80 J
Sol.16. (ABCD)
A
B1 kg
1 kg 4 m/s
4 m/s
1 kg C
After collision linear momentum of (A + C) system should be conservable in horizontal
direction.
2 kg
40
20
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A2 v 1 4
Av 2m / s
No horizontal force on B therefore no change in i t’s velocity.
Bv 4m / s
1 1 2 2 3 3com
1 2 3
m v m v m v ...... 1 4 1 4 1 0v
m m m 1 1 1
com
8v
3
2 m/s
4 m/s
8/3com
1/3
2/3
1 8w 2
3 3
w 2 rod / s
SECTION – 3 : (Comprehension Type)
Sol.17. (AB) Net force on system along horizontal directionxF 0
Hence linear momentum of system in horizontal direction will be conserved.
There is no non-conservative force on system. Therefore mechanical energy will be
conserved.
Sol.18. (A)
m
m2v
M 1v
initial
Initial Pi = 0 Pf = Mv1 + Mv2
TEi = mgh Pi = Pf 2 2
f 2 1
1 1TE mv Mv
2 2
1 2O Mv mv
2 1mv Mv ……. (1)
1
2
Mvv
m
i f TE TE
2 2
2 1
1 1mgh mv Mv
2 2
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2
211
Mv1 1mgh m Mv
2 m 2
Solving this 1
2ghv m
M m M
Sol.19. (ABD)
f
R
F
netF F ma
Fa
m (accelerate in forward direction)
F f ma
2f F R MR
a
R
f F R 2MR a
R
f F ma
F f
ma
Fa ; f 0
2m
netF F ma
Fa
m (Accelerate in forward direction)
nett FR (In clockwise direction)
Sol.20. (ABC)
f
F
F f ma
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fR I a
R
f R2MR
a
2 R
maf
2
maF ma
2
3maF
2
2Fa
3m
mf
2
2
F
3m
Ff
3
nett fR
PART II : CHEMISTRY
SECTION – 1 : (One Integer Value Correct Type)
Sol.21. (AC)
Sol.22. (BC) H mass heatcapacity T
500 4.18 20T.
This increase in temperature is balanced by addition of ice cubes of one molecule. Thus
number of moles of ice cubes.
1
500 4.18 2077
6.02 1000Jmol
Sol.23. (BC)
Sol.24. (C) using the expression
a
saltpH pK log
acid
We get 5 Salt
4.75 log 1.34 10 log0.02M
which gives salt
4.75 4.87 log0.02M
Or salt
0.02M=0.76 or 2salt 1.52 10 M
Hence, Amount of sodium propanoate to be added = 21.52 10 mol
The addition of 0.01 mol of hydrogen chloride convert the equivalent amount of sodium
propanoate into propanoic acid. Hence, We will have
1
1
0.0152 0.01 molLpH 4.87 log 4.87 log 0.173 4.87 0.76 4.11
0.02 0.01 molL
The pH of 0.01 molar HCl solution would be
pH log 0.01 2 .
Sol.25. (AC)
Sol.26. (B) Use G 2.303RTlogK
Sol.27. (BD)
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Sol.28. (BD)
0
eq
AB g A g B g
t 1 0 0
1 1 1t 1
3 3 3
2 1 1 4
n3 3 3 3
gn
A Bp
AB
n n PKn n
1
p
1 1
P 1 3P P P3 3 82 4 / 3 6 4 8 K
3
SECTION – 2 : (One or More Than One Option Correct Type)
Sol.29. (B)
Sol.30. (AC) The solubility of 2
Zn OH will be given as
2 2sp2
c24
Ks Zn Zn OH K OH
OH
The minimum solubility will be obtained by settingds
0d OH
Hencesp
c3
2K2K OH 0
OH
1/4 1/417
sp 5
c
2K 1.2 10OH 9.8 10
2K 0.13
pH 14 4.01 9.99
172
5 9
25
1.2 10s 0.13 9.8 10 2.5 10 M.
9.8 10
Sol.31. (A)
As p-derivative give only one product whereas o & m give more than one nitro
product.
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Sol.32. (ACD)
(A) In isothermal process, temperature is constant, therefore,
1 2T T
(C) w wisothermal adiabatic
Area under curve is greater for isothermal process, than that for adiabatic process.
(D)isothermal
U 0
For adiabatic process:
1TV constant
1 1
1 1 3 3T V T V
1
3 1
1 3
T V
T V
3 1T T hence internal energy will decrease.
i.e.,isothermal adiabaticU U
Sol.33. (ABD) Sol.34. (BCD) Sol.35. (ACD)
Sol.36. (ABD) dH dU PdV VdP
SECTION – 3 : (Comprehension Type)
Sol.37. (D) Sol.38. (C)Sol.39. (AC) Equilibrium is achieved at point – X. In graph A, at point X, the free energy of both reactants
and products are equal and G 0 which is the characteristic of reaction at equilibrium.
(B) Is not correct because equilibrium is achieved
(C) Is correct because free energy is minimum at X.
(D) Cannot be correct.
Sol.40. (BD) The reaction is reversible. The graph B tells that the reactants concentration are decreasing
while products concentration are increasing and after certain time, both the concentrations
are becoming constant which is a characteristic of reversible reaction which attains
equilibrium.
(A) is not correct because conc. Of reactant is not reaching zero
For (C) and (D) as
PK
R then K is less than 1. So (D) is correct.
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PART III : MATHEMATICS
SECTION – 1 : (One Integer Value Correct Type)
Sol.41. (C) y = (tanx sinx) y Now z = 3x z
y2 = (tan x – sin x) + y z
2 = x
3 + z
y =1 1 4(tanx sinx)
2
z =
31 1 4x
2
y > 0 z > 0
y =1 1 4(tanx sinx)
2
z =
31 1 4x
2
x 0lim
3
1 1 4(tanx sinx)1
2
1 1 4x1
2
=x 0lim
3
1 1 4(tanx sinx)
1 1 4x
Rationalization
=x 0lim
3
4(tanx sinx)
4x
×31 1 4x
1 1 4(tanx sinx)
=x 0lim
3
tanx sinx
x
×2
2
=x 0lim
sinx
x ×
2
1 cosx
x
= 1 × 1/2 = ½
Sol.42. (C) Let A = cosec –1
2 13x 1
4
+ sec
–1 2 13x
4
= cosec –1
2 11 3x
4
+ sec
–1 2 13x
4
where 3x2
+
1
4 1
Now A will be minimum when 2 13x
4
is minimum
2 13x
4
= 1
Amin = cosec –1
2 + sec –1
1 =6
hence12
A = 2
Sol.43. (AC) y = f(x) = 4x
3
– x
2
– 2x + 1
3
1
2
1
4
1,
2
1
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g(x) =
1f(x) ; 0 x
2
1f(1/ 2) ; x 1
2
3 x ; 1 x 2
So1
g4
=1
2 ;
3g
4
=1
4 ;
5g
4
= 3 – 5
4.
Sol.44. (AC)
–
–
– –
From graph it is clear that m 0,2
= 5
Sol.45. (CD)(a, 0)
(0, a)
( – a, 0)
|x| + |y| = a
x2 + y2 = a2
a|y||x|
(0, – a)
A1 area included between the line and circle in first quadrant
=2a 1
4 2
a
2 =
2( 2)a
4
A2 = area included between the line and
| x | + | y | = a
=1
2a
2 –
a2
0( a x ) dx
= (9 – 2)2a
12
Now 2
1
A 1
A 3
9 2
2
, A = 9, B = 1
A + B – 1 = 9
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y = 3 /16
Y
O X
Sol.46. (BD) Minimum (x1 – x2)2 + x1 (0, 2 )
This can be translate to finding minimum distance between two curves.
y = & y =
Minimum distance his along the common normal.
The normal passes through (0, 0) [as y = is a semicirle]
y1 = – mN = +
Equation of normal y – y2 = (x – x2)
Satisfies (0, 0)
9y2 = x23 9 × = x2
3 x2
4 = 81
x2 = ± 3 as x2 R+
x2 = 3 y2 = 3
Hence minimum distance = = 3 = 2
Given expression is the equation of minimum distance
(2)2 = 8
Sol.47. (D) Since given differential equation is
y (x + y3) dx = x (y3 – x) dy
(xy dx + x2 dy) + y4 dx – y3x dy = 0
x (y dx + x dy) + y3 (y dx – x dy) = 0
xd (xy) = y3 (x dy – y dx)
xd (xy) = x2y3 d
d
On integrating – + c
at (4, – 2)
+ c c = 0 y3 = –2x y = ( – 2x)1/3
Since y = g(x) =
= g (x) = x . sin 2x + x . ( – sin 2x) = 0
y = c1
(constant)
put sin x = cos x =
c1 = (sin –1 + cos –1) dt =
y = g (x) =
Hence area between y = and y = ( – 2x)1/3
= x dy
=
= sq. units.
2
2
21
x
9x2
21x2
1x
9
22x
9
9
x22
2x
9
233 22
2
xy
21
xy1
xsin
8/1
xcos
8/1
112 2
dttcosdttsin
dy2
y316/3
0
4
16
3.
8
1
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Sol.48. (AB) f() = .....(1)
x = dx = – dt
f() = =
....(2)
Equation (1) + (2)
2f() = = = 2 l n
Now g()
g() = dx = = 2 l n
f(200) – g(50) = l n(200) – l n(50) = l n 4 = 3 · l n 4
a+ b = 7
SECTION – 2 : (One or More Than One Option Correct Type)
Sol.49. (ACD) Diff. we get 2f(x) f (x) = f(x)
22sec x
4 tanx
f(x) 0, so f (x) =2sec x
4 tanx
f(x) = n (4 + tan x) + c
Given f(0) = n 4. So f(x) = n (4 + tan x).
Sol.50. (ABCD) (A) sgn (e –x)
e –x > 0 for every real x
every constant function is a periodic function.
(C) f(x) =8 8
1 cosx 1 cosx
=2
16
1 cos x =
4
|sinx|
= 4|cosec x|
this is a periodic function.
(D) f(x) =1
x2
+1
x2
+ 2[ – x]
dxx23
1xx
x3x2
1xxcot
x
1
1
2
2
21
t
12t
1
dt
t
1
t2t3
1tt
3t2
1ttcott
2
1
2
221
dt
t2t3
1tt
3t2
1ttcot
t
1
1 2
221
dtt3t2
1tt
t23
1ttcot
t
1
12
221
1 t
1
nn l l
dx1
|1x||1x|
|)2x)(1x(||2x3x|n
1n)x(f )x(f .e.ifunctionOdd
2
l
l
ln
1ln
dx.1
1nn l l
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–1, –3
64
6
(1,0)
=1
x2
+
1x
2
+ 2 [ – x]
=1 1 1 1
x x x x2 2 2 2
+ 2 ( – x – { – x})
= – 1
x2
–
1x
2
– 2 { – x}
Since { } is a periodic function hence this function is periodic. Sol.51. (AB) f(x) = [x]2 + [x + 1] – 3 = {[x] + 2} {[x] – 1}
So, x = 1, 1.1, 1.2, .... f(x) = 0 f(x) is many one
only integral values will be attained f(x) is into
Sol.52. (BD) f(x) =
2
2
x 2 , 1 x 2
x 2, 2 x 3
2
11, x 3
3
f (x) =2x , 1 x 2
x , 2 x 3
function is increasing in each of the two intervals (1, 2) and (2, 3) but not in [1, 3]
Clearly least value of f(x) is 3 and greatest value of f(x) does not exist.
Sol.53. (AB) Domain of sin –1
x and cos –1
x, each is [ –1, 1] and that of sec –1
x and cosec –1
x,
each is ( –, –1] [1, )
Domain of f(x) must be { –1, 1}
Range of f(x) will be {f( –1), f(1)}
where f( –1) = sin –1
( –1) · cos –1
( –1) · tan –1
( –1) · cot –1
( –1) · sec –1
( –1) · cosec –1
( –1)
= 3
· · · · ·2 4 4 2
=
63
64
and f(1) = 0 {as cos
–1 1 = 0}
(i) Thus, the graph of f(x) is a two point graph which
doesn't lie above x - axis (A) is correct statement
(ii) f(x)max= 0 and f(x)min =63
64
6
max min
3f(x) f(x)
64
(B) is correct statement
(iii) f(x) is one-one hence injective
(C) is incorrect statement
(iv) Domain is { –1, 1}
Number of non-negative integers in the domain of f(x) is one (D) is incorrect statement
Sol.54. (ACD)
Sol.55. (BD) (A) We have
x
1x 1 3
(t 1) sin t dtLim
(x 1)
0form
0
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=x 1 2
(x 1) sin xLim
3(x 1)
= x 1
sin x 0Lim
3(x 1) 0
= x 1
sin( x)Lim
3(x 1)
=
x 1
sin(1 x)Lim
3(x 1)
=x 1
sin (x 1)Lim
3 (x 1)
= (1)3
=
3
(B) We have 2x + y = 0, 4y + 3z = 24 and 12x – 7z = 24.
On solving, we get the point of intersection as ( – 12, 24, – 24) whose
distance from (0, 0, 0) is 36.
(C) We have1
2
sint
x g(x) dx = (1 – sin t) ........... (i)
Differentiating both the sides of (1) with respect to 't', we get
0 – sin2 t · g(sin t) · cos t = – cos t
g(sin t) =2
1
sin t ........... (ii)
Putting t =4
in (2),
We get g1
2
= 2
(D) We have
x2 y
2
3
12 3x
y2
33
3
2x y
4 x2y 4
Maximum value = 4
Sol.56. (AC) We have
I =a 1 x 1 x x
1 a 1 x 2x
sin e cos e edx
tan e tan e e 1
=
a x
1 a 1 x 2x
1 e. dx
2 (tan e tan e ) (e 1)
Put tan –1ex = t x
2x
edx
e 1 = dt
I =
1 atan e
1 a
0
dt
2 (t tan e )
=1 atan e
1 a
0ln(t tan e )
2
= 1 a 1 aln 2 tan e ln tan e2
= ln22
SECTION – 3 : (Comprehension Type)
Sol.57. & 58 (B & C)
f(x) =
n
nxlim cosn
=
n
nxlim 1 cos 1n
=n
xlim cos 1 n
ne
=
2
n
1 xlim 2sin n
2 ne
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=
2
n
1 x
2 n2 lim
1
ne
= n
x2 lim
2
x1 ne e
14
n
y = f(x) = e –x/2, x 0 range = (0, 1]
g(x) =xlim
(1 – x + x n e )n
=
1
n
n
( e 1)lim x
1/ne
= ex x R
h(x) = tan –1 (g –1 (f –1(x))
x
2 = ny x = 2n
1
y f –1(x) = 2n
1
x 0 < x 1
y = g(x) = ex
x = ny g –1(x) = nx
g –1 1
2 nx
= n 1
2 nx
for 0 < x < 1
h(x) = tan –1 2
1n n
x
for 0 < x < 1
Sol.59. (D) Let 0 < < < < 1, and , are the roots of
f(x) = x3 – 3x + k = 0 f() = f() = 0
f(x) satisfies RMVT f (c) = 0 3c2 = 0 c = ± 1
but c must be lies between & .
Hence k
Sol.60. (A) Let f(x) = tan –1x
then for some a (x, y), f () =1 1tan y tan x
y x
(LMVJ)
2
1
1 =
1 1tan x tan y
x y
1
|tan –1x – tan –1y| |x – y|
END OF Solution