Kinematics-02-OBJECTIVE SOLVED

OBJECTIVE SOLVED 1. Pick up the correct statements: (a) area under a – t graph gives velocity (b) area under a – t graph gives change is velocity (c) path of projectile as seen by another projectile is parabola (d) a body, whatever be its motion, is always at rest in a frame of reference fixed to body itself. Solution: dv  a dt v2   dv   a dt v1  v = Area under a – t graph where v = magnitude of change in velocity. The path of a projectile as seen by another projectile is a straight line becomes, the relative velocity between the particles remains constant.  (b) and (d) 2. The angular acceleration of a particle moving along a circular path with uniform speed is (a) uniform but non-zero (b) zero (c) variable (d) such as cannot be predicted from the given information. Solution: As angular speed of the particle is constant and hence angular acceleration is zero.  (b) 3. A particle is projected horizontally from the top of a cliff of height H with a speed of curvature of the trajectory at the instant of projection will (a) H/2 (b) H (c) 2H (d)  . Solution: Since, →  → . The radius Radial acceleration a r  g We know a  v2 / r v2   r g where r is the radius of curvature.  2gH  g r  r  2H ( v  2gH ) Hence (C) 4. A body when projected vertically up, covers a total distance D. During the time of its flight t. If there were no gravity, the distance covered by it during the same time is equal to (a) 0 (b) D (c) 2D (d) 4D. Solution: The displacement of the body during the time t as it attains the point of projection  S  0 t  2v 0 g  v 0 t  1 gt 2  0 2 During the same time t, the body moves in absence of gravity through a distance D  v0t , because in absence of gravity g = 0   2v 0  2v 2  D  v 0    0 ...(i)  g  g In presence of gravity the total distance covered is v 2 v 2  D  2H  2 0  0 ...(ii) 2g g (i)  (ii)  D  2D Hence (c) 5. A particle is projected from point P with velocity 5 2ms1 perpendicular to the surface of a hollow right angle cone whose axis is vertical. It collides at Q normally. The time of the flight of the particle is (a) 1 sec. (b) sec. (c) Solution: t  2 2 sec u  5 2  2  1sec. (d) 2 sec. g sin  10 Hence (a) x 6. The relative velocity of a car ‘A’ with respect to car B is 30 2 m/s due North-East. The velocity of car ‘B’ is 20 m/s due south. The relative velocity of car ‘C’ with respect to car ‘A’ is 10 2 m/s due North-West. The speed of car C and the direction (in terms of angle it makes with the east). (a) 20 m/s, 45º (b) 20 2m / s, 135º (c) 10 Solution: m / s, 45º (d) 10 2 m / s, 135º . Given →  30 2ms1 | vAB | | vB | 20 ms → 1 | vCA | 10 2 ms Now → → → ˆ ˆ E(x) vAB  vA  vB  30 2(cos 45º i  sin 45º j) or, → → vA vB  (30iˆ  30ˆj)ms1 ...(i) vB and, →  (20ˆj)ms1 ...(ii) and → → → ˆ ˆ vCA  vC  vA  10 2 (cos 45º i  sin 45º j) or vC →  (10iˆ  10ˆj)ms1 ...(iii) solving equation (i) (ii) and (iii) we’ll get →  20ˆi  20ˆj (a) 7. Two particles 1 and 2 are allowed to descend on the two frictionless chord OA and O OB of a vertical circle, at the same instant from point O. The ratio of the velocities of the particles 1 and 2 respectively, when they reach on the circumference will be 1  (OB is the diameter) 2 (a) sin  (b) tan  (c) Solution: cos  OA  d cos , a OA  g cos  (d) none of these. A B Along OA O 2  2g cos .d cos  1  Along OB v 2  2gd 2 d g cos v A  v B A  cos  B Hence, C is correct. 8. A ball is dropped vertically from a height d above the ground. If it hits the ground and bounces up vertically to a height d/2. Neglecting subsequent motion and air resistance, its velocity v varies with the height h above the ground as (a) (b) (c) (d) . Solution: As the ball falls, at height h the velocity of the ball is zero and at any height with decreasing h, v increases. When h = 0, v = velocity is maximum. h, v 2  u 2  2g(d  h) , After the ball collides the floor, its velocity changes in magnitude as wall as direction, as the body goes to a smaller height in bouncing up .The change in velocity takes place within zero height and with no change in time. Hence, (a) is correct choice. 9. A particle moves along a straight line according to the law S2  at 2  2bt  c . The acceleration of the particle varies as (a) (c) Solution: S3 S2 (b) (d) S2 / 3 S5 / 2 . S  (at 2  2bt  c)1/ 2 Differentiating, dS  1 (at 2  2bt  c)1/ 2  (2at  2b)  at  b dt 2 at 2  2bt  c   a  (at  b)(at  b) d 2S    at 2  2bt  c dt 2  d 2S 1 (at 2  2bt  c)  (ac  b2 ) S S2  dt 2  S3  acceleration  S3  (a) 10. A car accelerates from rest at a constant rate  for some time, after which it decelerates at a constant rate  to come to rest. If the total time elapsed is t, the maximum velocity acquired by car is (a) (c) Solution: V   t (  ) V  2 t (  ) (b) (d) V   t (  ) V  2 t (  ) From motion from A to B V  t1 or t  V 1  V From motion from B to C 0  V  t 2 or t 2   A B C  t  t  t  V  V  V(  ) 1 2    V   t (  )  (a) 11. A stone A is dropped from rest from a height h above the ground. A second stone B it simultaneous y thrown vertically up from a point on the ground with velocity v. The line of motion of both the stones is same. The values of v which would enable the stone B to meet the stone A midway between their initial positions is (a) 2 gh (b) 2 (c) Solution: Time of travel of each stone = (d) . Distance travelled by each stone  h 2 For stone A, h  1 gt2 2 2 h 1 i.e., 2 t  1  h  For stone B,  ut  gt  u  g   or, 2 2 h  u  h 2 2 u  h 2  g   u  h g  h The correct option is (c) 12. A stone is dropped from rest from the top of a cliff. A second stone is thrown vertically down with a velocity of 30 m/s two seconds later. At what distance from the top of a cliff do they meet? (a) 60 m (b) 120 m (c) 80 m (d) 44 m. Solution: The two stones meet at distance S from top of cliff t seconds after first stone is dropped. For 1st stone S  1 gt 2 ; 2 For 2nd stone S  u(t  2)  1 g(t  2)2 . 2 i.e., 1 gt 2  ut  2u  1 gt 2  2gt  2g 2 2 0  (u  2g)t  2(u  g); t  2(u  g)  2(30  10)  4s u  2g 30  20 Distance S at which they meet  1  gt 2  1 10 16 2 2 = 80 m from top of cliff  (c) 13. A particle is projected from a point O with velocity u in a direction making an angle  upward with the horizontal. At P, it is moving at right angles to its initial direction of projection. Its velocity at P is (a) (c) u tan  u cos ec (b) (d) u cot  u sec  . P  (90º-) Solution: v cos(90  )  v sin   u cos ; v  u cot  90º u v  (b) O  14. A man running at 6 km/hr on a horizontal road observes that the rain hits him at an angle of 30º from the vertical. The actual velocity of rain has magnitude (a) 6 km/hr (b) 6 km/hr (c) 2 km/hr (d) 2 km/hr Solution: → VR → VRM  velcoity of rain VM  velocity of rain relative to man → VM  velocity of man Given, VM  6 kmh-1, VRM  at angle 30º from vertical → → → here VR  VRM  VM from figure, VM tan 30º  VM VR  6 VR  VR  6 km/hr  (b) 15. The angular acceleration of a particle moving along a circular path with uniform speed is (a) uniform but non-zero (b) zero (c) variable (d) such as cannot be predicted from the given information. Solution: As angular speed of the particle is constant and hence angular acceleration is zero.  (b)

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