It is very important to have the idea of any examination to get success in that. The best way to have that idea is to have a look at previous year Questions of that examination. That's why we have collected some previous year Questions with Solutions of JEE Main, JEE Advance, NEET, IIT JEE, AIEEE, AIIMS, WBJEE, EAMCET, Karnataka CET, CPMT, Kerala CET, MP PMT and Other State JE Exams so that you can get clear pattern and level of question that will be asked in forthcoming JEE Main, JEE Advance, NEET, IIT JEE, AIEEE, AIIMS, WBJEE, EAMCET, Karnataka CET, CPMT, Kerala CET, MP PMT and Other State JE Exams.
JEE Previous Year's Questions With Solutions
1. The relation between time t and
distance x is t = ax2 + bx where a and b are constants. The
acceleration is: (AIEEE 2005)
(A) – 2av2
(B) 2av3
(C) – 2av3
(D) 2av2.
Sol: (C)
Given: t = ax2 + bx --------- (1)
Differentiate the equation (1) w.r.t. ‘t’
We get, 1 = 2ax (dx/dt) + b(dx/dt)
Or, 1 = 2axv + bv [since v = (dx/dt)]
Or, v = 1/ (2ax +b) -------- (2)
Again, differentiate the equation (2) w.r.t. ‘t’
We get, (dv/dt) = – 2av3.
So, acceleration = – 2av3.
2. A projectile can have the same range
R for two angle of projection. If t1 and t2 be the time
of flights in the two cases, then the product of the two time of flights is
proportional to: (AIEEE 2005, 2004, Karnataka CET 2003, EAMCET 2012)
(A) R
(B) 1/R
(C) 1/R2
(D) R2.
Sol: (A)
Range is same for angle of projection θ and (90 – θ).
Range, R = (u2 sin 2θ)/g
Time of flight for 1st case:
→ t1 = (2u sin θ)/g
And, Time of flight for 2nd case:
→ t2 = {2u sin (90 – θ)}/g
A.T.Q. t1.t2 = (4u2 sin θ
cos θ)/g2
Or, t1.t2 = (2/g) {(u2 sin 2θ)/g}
= 2R/g.
Therefore, t1.t2 is proportional to R.
3. A particle located at x = 0 at time
t = 0, starts moving along the positive x-direction with a velocity v that
varies as v = α√x. The displacement of the particle varies with time as: (AIEEE 2006)
(A) t
(B) t1/2
(C) t3
(D) t2.
Sol: (D)
Given: Velocity, v = α√x
Or, dx/dt = α√x
Or, dx/√x = α dt ------- (1)
Integrating equation (1)
We get, 2x1/2 = αt + c
At t = 0, x = 0 → c = 0.
So, x = (αt)2/4.
Hence, the displacement of the particle varies with time as t2.
4. The velocity of a particle is v = v0
+ gt + ft2. If its position is x = 0 at t = 0, then its displacement
after unit time (t = 1) is: (AIEEE 2007)
(A) v0 + g/2 + f
(B) v0 + 2g + 3f
(C) v0 + g + f
(D) v0 + g/2 + f/3.
Sol: (D)
Given: Velocity, v = v0 + gt + ft2
Or, dx/dt = v0 + gt + ft2
Or, dx = (v0 + gt + ft2) dt ------- (1)
Integrating equation (1)
We get, x = v0t + gt2/2 + ft3/3
+ c
At t = 0, x = 0 → c = 0.
So, x = v0t + gt2/2 + ft3/3.
Displacement (t = 1) = v0 + g/2 + f/3.
5. A body starts from rest at time t =
0, the acceleration time graph is shown in the figure. The maximum velocity
attained by the body will be: (IITJEE
2004)
(A) 55 m/s
(B) 110 m/s
(C) 550 m/s
(D) 650 m/s.
Sol: (A)
Area under the curve in acceleration-time graph gives the
change in velocity.
Therefore, ΔV = ½ * 10 * 11 = 55 m/s.
Since initial velocity = 0.
Therefore maximum velocity attained = 55 m/s.
6. If the displacement of a particle
changes with time as √x = t + 3, then the velocity of the particle will be
proportional to: (WBJEE 2007)
(A) t–1
(B) t
(C) √t
(D) t–2.
Sol: (B)
Given: √x = t + 3
Or, x = (t + 3)2
Or, dx/dt = 2 (t + 3)
Therefore, the velocity of the particle is proportional
to t.
7. The distance travelled by an object
along a straight line in time ‘t’ is given by S = 3 – 4t + 5t2, the
initial velocity of the object is: (WBJEE
2008)
(A) 3 unit
(B) – 3 unit
(C) 4 unit
(D) – 4 unit.
Sol: (D)
Given: S = 3 – 4t + 5t2
Velocity, V = ds/dt = – 4 + 10t
Velocity, V (t = 0) = – 4 unit.
8. A body is fired vertically upwards.
At half the maximum height, the velocity of the body is 10 m/s. The maximum
height raised by the body is (g = 10 m/s–2): (Odisha JEE 2008)
(A) 10 m
(B) 15 m
(C) 20 m
(D) Zero.
Sol: (D)
Taking motion of the body from half the max height upto the highest
point, we have u = 10 m/s, v = 0, a = – 10 m/s–2, s = h/2.
We know, v2 – u2 = 2as
Or, 02 – 102 = 2 * (– 10) * (h/2)
Or, h = 10 m.
Hence, the maximum height raised by the body is 10 m.
9. A ball is projected horizontally
with a velocity of 5 m/s from the top of a building 19.6 m high. How long will
the ball take of hit the ground? (WBJEE
2010)
(A) √2 s
(B) 2 s
(C) 3 s
(D) √3 s
Sol: (B)
Given: ux = 5 m/s, uy = 0, H = – 19.6 m,
a = – 9.8 m/s2.
Equation of motion along Y-axis:
We have, H = uyt + ½ at2
Or, – 19.6 = 0 – ½ * 9.8 * t2
Or, t = 2s.
10. A bullet moving with a speed of 100
m/s can just penetrate two planks of equal thickness. Then, the number of such
planks penetrated by the same bullet when the speed is doubled will be: (Karnataka CET 2004)
(A) 8
(B) 6
(C) 10
(D) 4
Sol: (A)
Given: initial speed, u = 100 m/s; final speed, v = 0.
Assume: thickness of plank be x.
We have, v2 – u2 = 2as
Or, 02 – 1002 = 2a * (2x)
Or, a = – 2500/x.
Now, initial speed, u = 200 m/s; v = 0; s = nx.
Again, v2 – u2 = 2as
Or, 02 – 2002 = 2 * (– 2500/x) * (nx)
Or, n = 8.
11. A metro train starts from rest and
in five seconds achieves 108 km/h. After that is moves with constant velocity
and goes to rest after travelling 45 m with uniform retardation. If total
distance travelled is 395 m, find total time of travelling: (UPSEE 2006)
(A) 15.3 s
(B) 12.2 s
(C) 17.2 s
(D) 9 s
Sol: (C)
For 1st 5 s.
Initial velocity, u = 0; final velocity, v = 108 km/h = 30
m/s; t1 = 5s.
We have, v = u + at
Or, 30 = 0 + a * 5
Or, a = 6 m/s.
So, distance travelled, s = ut + ½ at2
Or, s = 75 m.
Let distance travelled with constant velocity be x.
→ 75 + x + 45 = 395
Or, x = 275 m.
And, time taken t2 = 275/30 = 9.2 s.
For last 45 m:
Initial velocity, u = 30 m/s; final velocity, v = 0; s = 45
m.
We have, v2 – u2 = 2as
Or, 02 – 302 = 2 * a * 45
Or, a = – 10 m/s2.
Time taken in travelling 45 m is
→ t3 = (v – u)/a
Or, t3 = 3 s.
So, total time taken in whole journey = t1 + t2
+ t3 = 5 + 9.2 + 3 = 17.2 s.
12. A projectile is thrown in the upward
direction making an angle of 600 with the horizontal direction with
a velocity of 147 m/s. then the time after which its inclination with the
horizontal is 450, is? (UPSEE
2006)
(A) 2.745 s
(B) 15 s
(C) 5.49 s
(D) 10.98 s
Sol: (C)
During the projectile motion, horizontal component of
velocities at different point of projectile motion remain same.
So, u Cos 600 = v Cos 450
Or, 147 * ½ = v * 1/√2
Or, v = 147/√2 m/s.
Vertical component of initial velocity is
→ uy = u sin 600 = 147√3/2 m/s
Vertical component of velocity @ 450 is
→ vy = v sin 450 = (147/√2) (1/√2) =
147/2 m/s.
We have, vy = uy + at
Or, 147/2 = 147√3/2 – 9.8t
Or, t = 5.49 s.
13. A particle moves in a straight line
with retardation proportional to its displacement. Its loss of kinetic energy
for any displacement x is proportional to: (UPSEE 2007)
(A) log ex
(B) x2
(C) ex
(D) x
Sol: (B)
Given: retardation, – a = kx
Where, k = proportionality constant and x = displacement.
Now, dv/dt = – kx
Or, (dv/dx) (dx/dt) = – kx
Or, v (dv/dx) = – kx
Or, v dv = – kx dx
Integrating both side we get,
→ v2/2 = – kx2/2 + c
Or, K.E. = mv2/2 = – mkx2/2 + mc
So, loss of kinetic energy for any displacement x is proportional
to x2.
14. A ball thrown by one player reaches
the other in 2 s. The maximum height attained by the ball above the point of
projection will be (g = 10 m/s2): (UPSEE 2008)
(A) 5 m
(B) 10 m
(C) 2.5 m
(D) 7.5 m
Sol: (A)
Given: time of flight, T = 2 s.
We have, T = (2u sin θ)/g
Or, 2 = (2u sin θ)/g
Or, u sin θ = g.
And, max height H = (u2 sin2 θ)/2g
Or, H = g2/2g = g/2 = 5 m.
15. A ball is dropped from a bridge at a
height of 176.4 m over a river. After 2s, a second ball is thrown straight
downwards. What should be the initial velocity of the second ball so that both
hit the water simultaneously? (UPSEE
2009)
(A) 14.5 m
(B) 49 m/s
(C) 2.45 m/s
(D) 24.5 m/s
Sol: (D)
For 1st ball: H = – 176.4 m; u = 0; a = – g.
We have, H = ut + ½ at2
Or, – 176.4 = 0 – ½ gt2
Or, t = 5.9 s.
For 2nd ball: t = 5.9 – 2 = 3.9 s; H = – 176.4 m;
initial velocity, u = – u0; a = – g.
Again, H = ut + ½ at2
Or, – 176.4 = – u0 * 3.9 – ½ * g * 3.92
Or, u0 = 24.5 m/s.
16. A bullet is fired with a velocity u
making an angle of 600 with the horizontal plane. The horizontal
component of the velocity of the bullet when it reaches the maximum height is:
(WBJEE 2009)
(A) 0
(B) u
(C) (√3/2) u
(D) u/2
Sol: (D)
Horizontal component of the velocity in a projectile motion
remains constant.
Horizontal component of the velocity = u cos θ = u cos 600
= u/2.
17. A bullet emerges from a barrel of
length 1.2 m with a speed of 640 m/s. Assuming constant acceleration, the
approximate time that it spends in the barrel after the gun is fired is: (WBJEE 2008)
(A) 40 ms
(B) 4 ms
(C) 1ms
(D) 400 ms.
Sol: (B)
Given: u = 0; v = 640 m/s; s = 1.2 m.
Find: a =? t =?
We have, v2 – u2 = 2as
Or, 6402 – 02 = 2 * a * 1.2
Or, a = 6402/2.4 m/s2.
And, t = (v – u)/a
Or, t = (640 – 0)/ (6402/2.4)
Or, t = 0.00375 s ≈ 0.004 s = 4 ms.
18. A particle is projected at 60° to
the horizontal with a kinetic energy K. The kinetic energy at the highest point
is: (WBJEE 2009, WBJEE 2012)
(A) K
(B) Zero
(C) K/4
(D) K/2
Sol: (C)
Let mass of particle be m and velocity of projection v.
Given: kinetic energy = K = ½ mv2
Velocity at the highest point = v cos 600 = v/2.
So, kinetic energy at the highest point = ½ m (v/2)2
= (½ mv2)/4 = K/4.
19. A scooterist sees a bus 1 km ahead
of him moving with a velocity of 10 m/s. With what speed the scooterist should
move so as to overtake the bus in 100 s? (Odisha JEE 2008)
(A) 10 m/s
(B) 50 m/s
(C) 20 m/s
(D) 30 m/s.
Sol: (C)
Distance travelled by bus in 100 s = 10 * 100 = 1000 m.
Let speed of scooter be u m/s.
Distance travelled by scooter in 100 s = u * 100 = 100u.
A.T.Q, 1000 + 1000 = 100u
Or, u = 20 m/s.
20. The maximum range of projectile
fired with some initial velocity is found to be 1000 m, in the absence of wind
and air resistance. The maximum height reached by the projectile is: (Odisha JEE 2009)
(A) 250 m
(B) 1000 m
(C) 500 m
(D) 2000 m.
Sol: (A)
We have, max range Rmax = u2/g [for max
range θ = 450]
Or, 1000 = u2/10
Or, u = 100 m/s.
And max height H = (u2 sin2 θ)/2g
Or, H = (1002 sin2 450)/ (2*10)
Or, H = 250 m.
21. A car starting from rest,
accelerates at the rate f through a distance s, then continues at constant
speed for time t and then decelerates at the rate f/2 to come to rest. If the
total distance traversed is 15 s, then: (AIEEE
2005)
(A) s = ½ ft2
(B) s = 1/4 ft2
(C) s = 1/72 ft2
(D) s = 1/6 ft2.
Sol: (C)
For 1st part of journey: u1 = 0; a1
= f; s1 = s; t1 = t1.
Distance travelled, s1 = u1t1
+ a (t1)2
Or, s = ½ f (t1)2 -------- (1)
And (v1)2 – (u1)2
= 2a1s1
Or, v1 = √ (2fs) = ft1.
For 2nd part of journey: velocity is constant (v2
= v1); t2 = t.
Distance travelled, s2 = v1t2
Or, s2 = f t1 t
For 3rd part of journey: v3 = 0; a3
= – f/2; u3 = v1 = ft1.
Again, (v3)2 – (u3)2
= 2a3s3
Or, – (ft1)2 = 2 (– f/2) s3
Or, s3 = f (t1)2 = 2s.
A.T.Q, s1 + s2 + s3 = 15s
Or, s + f t1 t + 2s = 15s
Or, f t1 t = 12s --------- (2)
From equation (1) & (2)
We get, t1 = t/6.
So, s = ½ f(t1)2 = ½ f (t/6)2
= s = 1/72 ft2.
22. A ball is released from the top of a
tower of height h metres. It takes T seconds to reach the ground. What is the
position of the ball at T/3 second? (AIEEE
2004)
(A) 7h/9 metre from the ground
(B) 17h/18 metre from the ground
(C) 8h/9 metre from the ground
(D) h/9 metre from the ground.
Sol: (C)
We have, s = ut + ½ at2
Given: s = – h, t = T.
Therefore, – h = 0 – ½ gT2
Or, gT2 = 2h -------- (1)
After T/3 sec,
→ – h’ = 0 – ½ g (T/3)2
Or, h’ = gT2/18 -------- (2)
From equation (1) and (2)
We get, h’ = h/9.
Therefore, height of ball from ground = h – h’ = 8h/9.
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