Galileo writes that for angles of projection of a projectile at angles and , the horizontal ranges described by the projectile are in the ratio of (if )
1. 2 : 1
2. 1 : 2
3. 1 : 1
4. 2 : 3
A projectile thrown with a speed v at an angle θ has a range R on the surface of earth. For same v and θ, its range on the surface of moon will be (acceleration due to gravity on moon=):
(1) R/6
(2) 6 R
(3) R/36
(4) 36 R
A ball is projected with kinetic energy E at an angle of 45° to the horizontal. At the highest point during its flight, its kinetic energy will be
(1) Zero
(2)
(3)
(4) E
At the top of the trajectory of a projectile, the magnitude of the acceleration is
(1) Maximum
(2) Minimum
(3) Zero
(4) g
A body is projected at such an angle that the horizontal range is three times the greatest height. The angle of projection is
(1)
(2)
(3)
(4)
Two bodies are projected with the same velocity. If one is projected at an angle of 30° and the other at an angle of 60° to the horizontal, the ratio of the maximum heights reached is
(1) 3 : 1
(2) 1 : 3
(3) 1 : 2
(4) 2 : 1
If the range of a gun that fires a shell with muzzle speed v is R, then the angle of elevation of the gun is
(1)
(2)
(3)
(4)
If a body A of mass M is thrown with a velocity v at an angle of 30° to the horizontal and another body B of the same mass is thrown with the same speed at an angle of 60° to the horizontal. The ratio of horizontal range of A to B will be
(1) 1 : 3
(2) 1 : 1
(3)
(4)
Four bodies P, Q, R and S are projected with equal velocities having angles of projection 15o, 30o, 45o and 60o with the horizontal respectively. The body having the shortest range is?
1. | P | 2. | Q |
3. | R | 4. | S |
A stone projected with a velocity u at an angle θ with the horizontal reaches maximum height H1. When it is projected with velocity u at an angle with the horizontal, it reaches maximum height H2. The relation between the horizontal range of the projectile R and H1 & H2 is:
1. | \(R=4 \sqrt{H_1 H_2} \) | 2. | \(R=4\left(H_1-H_2\right) \) |
3. | \(R=4\left(H_1+H_2\right) \) | 4. | \(R=\frac{H_1{ }^2}{H_2{ }^2}\) |