“Men often become what they believe themselves to be. If I believe I cannot do something, it makes me incapable of doing it. But when I believe I can, then I acquire the ability to do it even if I didn’t have it in the beginning.”

– Mahatma Gandhi

Today we will discuss a few questions (MCQ) involving kinematics and elastic collision. The first four questions are relevant to AP Physics B as well as AP Physics C while the last question is relevant to AP Physics C.

(1) A particle moves from point A to point B (Fig.) in 2 seconds, covering three quarters of a circle of radius 1 m. What is the magnitude of the average velocity of the particle?

(a) 0.5 ms^{–1}

(b) 1 ms^{–1}

(c) √2 ms^{–1}

(d) 1/√2 ms^{–1}

(e) 2√2 ms^{–1}

The displacement of the particle during 2 seconds is equal to the length of the straight line AB. Since OA and OB have the same length of 1 m, AB = √2 m (length of the hypotenuse of the right angled triangle AOB.

Therefore average velocity = (√2)/2 = 1/√2 ms^{–1}

(2) A small object initially at rest starts sliding down from point P (Fig.) on a perfectly smooth inclined plane of inclination (θ) 30º and collides normally and elastically with the surface A of a large fixed block. If the distance PA (measured along the incline) is 2.5 m, what is the time taken by the object to traverse this distance? (g = 10 ms^{–2})

(a) 0.25 s

(b) 0.5 s

(c) 1 s

(d) 1.25 s

(e) 1.5 s

The motion of the object down the plane is uniformly accelerated and you can use the equation,

*s = ut + *½ *at*^{2} with usual notations.

Here displacement *s = *2.5* *m, *u = *0 and *a *= g sinθ = 10 sin30º = 5 ms^{–2}, which is the component of gravitational acceleration down the incline. Therefore we have

2.5 = 0 + ½ ×5 × *t*^{2}* *

This gives *t =* 1 s.* *

(3) In the above question, after starting from the point P, the minimum time required for the object to return to P is

(a) 0.5 s

(b) 1 s

(c) 1.5 s

(d) 2 s

(e) 2.5 s

Because of the elastic collision with the block, the velocity of the small object gets reversed. It travels up the incline for 1 seccond covering the distance of 2.5 metre and momentarily comes to rest. The times required for the trips down the inclined plane and up the inclined plane are equal since the acceleration is g sinθ throughout the motion. Therefore, after starting from the point P, the minimum time required for the object to return to P is

1 s +1 s = 2 s.

(4) In question No.2 suppose the inclined plane is not perfectly smooth, but offers a small frictional resistance. The object slides downwards from point P and collides with the block *elastically *after time *t*_{1}. It then slides upwards and momentarily comes to rest after an additional time *t*_{2}. Which one among the following statements is correct?

(a) *t*_{1} is less than 1 s

(b) *t*_{1}* = t*_{2} = 1 s

(c) *t*_{1}* = t*_{2}

(d) *t*_{1} is less than* t*_{2}

(e) *t*_{1} is greater than* t*_{2}

During the downward trip the acceleration has magnitude less than g sinθ since the frictional force opposes the motion of the object. In solving question No.2 we have found that the time for the downward trip is 1 second when the downward acceleration has magnitude g sinθ, appropriate to the case of a perfectly smooth incline. Since the magnitude of the downward acceleration is reduced in the case of an inclined plane that offers frictional resistance, the time required for the downward trip is *increased*.

During the upward trip (after colliding with the block) the deceleration has magnitude greater than g sinθ since the frictional force as well as gravity oppose the motion of the object. The object therefore comes to rest in a shorter time.

Therefore *t*_{1} is greater than* t*_{2} [Option (e)].

[When you project a ball up, the time of ascent will be equal to time of descent only if the air resistance is negligible. If the air resistance is not negligible, you will find that the time of ascent is less than the time of descent].

*The following question is specifically meant for **AP Physics C** aspirants:*

(4) A small object initially at rest at point P (Fig.) on a perfectly smooth inclined plane of inclination (θ) 30º starts sliding down under gravity and collides normally and elastically with the surface A of a large block that is projected up the incline. Assume that the mass of the small object is negligible compared to the mass of the block. If the distance PA (measured along the incline) and the velocity of the block up the incline at the instant of collision are 2.5 m and 2 ms^{–1} respectively, what will be the velocity of the small object immediately after the collision? (g = 10 ms^{–2})

(a) 5 ms^{–1}

(b) 7 ms^{–1}

(c) 9 ms^{–1}

(d) 3 ms^{–1}

(e) 2 ms^{–1}

In the case of an elastic collision the relative velocity after the collision is *equal and opposite* to the relative velocity before the collision:

*u*_{1 }– *u*_{2 }= –(*v*_{1 }– *v*_{2})…………(i)

At the instant of collision the large block moves *up the incline* with velocity 2 ms^{–1}. (Let us take this direction as *positive*). Or, *u*_{1 }= 2 **ms**^{–1}.

The velocity of the small object at the moment of collision is down the incline and hence *negative*. Its magnitude is 5 ms^{–1} as is obtained from the equation *v*^{2} = *u*^{2} + 2*as*:

*v*^{2} = 0^{2} + 2 g sinθ × 2.5 = 2×10 sin30º × 2.5 = 25 from which *v =* 5 ms^{–1} * *

Therefore, *u*_{2} = – 5** ms**^{–1} * *

The relative velocity before collision is *u*_{1 }– *u*_{2} = 2 – (–5)

The relative velocity after collision is (*v*_{1 }– *v*_{2}) = 2 – *v*_{2 }where *v*_{2} is the velocity of the small object just after the collision. (The velocity of the large block after collision is unchanged since its mass is large compared to the mass of the small object. Or, *v*_{1} = *u*_{1})

Therefore, from Eq (i) we have

2 – (–5) = –(2_{ }– *v*_{2})

This gives *v*_{2} = 9 ms^{–1}.

[You can obtain *v*_{2} by solving the following equations highlighting the conservation of momentum and kinetic energy in the case of elastic collisions:

*m*_{1}*u*_{1} **+ ** *m*_{2}*u*_{2} = *m*_{1}*v*_{1} **+ ** *m*_{2}*v*_{2}………………………..(i)

½ *m*_{1}*u*_{1}^{2} + ½ *m*_{2}*u*_{2}^{2} = ½ *m*_{1}*v*_{1}^{2} + ½ *m*_{2}*v*_{2}^{2}…………..(ii)

Equations (i) and(ii) can be solved for the velocities *v*_{1} and* v*_{2} of the block and the small object respectively after the collision. You will get

*v*_{1} = [(*m*_{1}–* m*_{2})*u*_{1} **+** 2*m*_{2}*u*_{2}] /(*m*_{1}+*m*_{2}) and

*v*_{2} = [(*m*_{2}–* m*_{1})*u*_{2} **+** 2*m*_{1}*u*_{1}] /(*m*_{1}+*m*_{2})

Here *m*_{1} >>* m*_{2}, *u*_{1} = 2 ms^{–1} and *u*_{2} = – 5 ms^{–1 }so that

*v*_{1} ≈ *u*_{1} = 2 ms^{–1} and

*v*_{1} ≈ –*u*_{2} + 2* u*_{1} = – (– 5) + (2×2) = 9 ms^{–1}

* * * * * * * * * * * * * * * * * * * * * * *

If you would like just arguments (without using lengthy mathematical steps, you may proceed like this (after obtaining the velocity of the object just before collision as –5 ms^{–1}):

Before collision the block has velocity 2 ms^{–1} where as the small object has velocity –5 ms^{–1} (relative to the ground). If the block is taken to be at rest for convenience, you have to imagine that the small object is moving towards the block with a velocity of –7 ms^{–1}. We are in fact using a frame of reference in which the block is at rest and are finding the velocities of the block and the small object in this frame by adding a velocity of –2 ms^{–1 }to both:

2–2 = 0 and –5–2 = –7.

Just after the elastic collision, the velocity of the object becomes 7 ms^{–1} relative to the block which we kept at rest for the convenience of argument. Our frame of reference is to be brought back to the ground. For this we add a velocity of +2 ms^{–1 }to the block and the small object and obtain the velocity of the block as 2 ms^{–1} (0+2 = 2) and the velocity of the small object as 9 ms^{–1} (7+2=9)].