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1: In order to describe motion of the stone once it is released, we realize that it would be easier for us if we shift the origin to the point where stone is released. Considering origin at the point of release and upward direction as positive as shown in the figure, the displacement during the motion of stone is :

y = OB = - 40 m

Motion under gravity

2: Distance, on the other hand, is equal to :

s = OA + AO + OB = 2 OA + OB

In order to obtain, OA, we consider this part of rectilinear motion (origin at the point of release and upward direction as positive as shown in the figure).

Here, u = 10 m/s; a = -10 m / s 2 and v = 0. Applying equation of motion, we have :

v 2 = u 2 + 2 a y y = v 2 - u 2 2 a = 0 2 - 10 2 - 2 x 10 = 5 m

Hence, OA = 5 m, and distance is :

s = 2 OA + OB = 2 x 5 + 40 = 50 m

3: The time of the journey of stone after its release from the balloon is obtained using equation of motion (origin at the point of release and upward direction as positive as shown in the figure).

Here, u = 12 m/s; a = -10 m / s 2 and y = - 40 m.

y = u t + 1 2 a t 2 - 40 = 10 t - 0.5 x 10 t 2 5 t 2 - 10 t - 40 = 0

This is a quadratic equation in “t”. Its solution is :

5 t 2 + 10 t - 20 t - 40 = 0 5 t ( t + 2 ) - 20 ( t + 2 ) = 0 ( 5 t - 20 ) ( t + 2 ) = 0 4 , - 2 s

As negative value of time is not acceptable, time to reach the ground is 4s.

It is important to realize that we are at liberty to switch origin or direction of reference after making suitable change in the sign of attributes.

Position

We use the equation Δ x = x 2 - x 1 = u t + 1 2 a t 2 normally in the context of displacement, even though the equation is also designed to determine initial ( x 1 ) or final position ( x 2 ). In certain situations, however, using this equation to determine position rather than displacement provides more elegant adaptability to the situation.

Let us consider a typical problem highlighting this aspect of the equation of motion.

Problem : A ball is thrown vertically from the ground at a velocity 30 m/s, when another ball is dropped along the same line, simultaneously from the top of tower 120 m in height. Find the time (i) when the two balls meet and (ii) where do they meet.

Solution : This question puts the position as the central concept. In addition to equal time of travel for each of the balls, rhe coordinate positions of the two balls are also same at the time they meet. Let this position be “y”. Considering upward direction as the positive reference direction, we have :

Vertical motion under gravity

The balls have same coordinate value when they meet.

For ball thrown from the ground :

u = 30 m / s , a = - 10 m / s 2 , y 1 = 0 , y 1 = y

y 2 - y 1 = u t + 1 2 a t 2 y - 0 = 30 t - 1 2 10 x t 2

y = 30 t - 5 x t 2

For ball dropped from the top of the tower :

u = 0 m / s , a = - 10 m / s 2 , y 1 = 120 , y 2 = y

y 2 - y 1 = u t + 1 2 a t 2

y - 120 = - 5 x t 2

Now, deducting equation (2) from (1), we have :

30 t = 120 t = 4 s

Putting this value in equation – 1, we have :

y = 30 x 4 - 5 x 4 2 = 120 - 80 = 40 m

One interesting aspect of this simultaneous motion of two balls is that the ball dropped from the tower meets the ball thrown from the ground, when the ball thrown from the ground is actually returning from after attaining the maximum height in 3 seconds. For maximum height of the ball thrown from the ground,

Vertical motion under gravity

When returning from the maximum height, the ball thrown up from the ground is hit by the ball dropped from towers.

u = 30 m / s , a = - 10 m / s 2 and v = 0

v = u + a t = 30 - 10 t t = 3 s

This means that this ball has actually traveled for 1 second (4 – 3 = 1 s) in the downward direction, when it is hit by the ball dropped from the tower!

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Source:  OpenStax, Physics for k-12. OpenStax CNX. Sep 07, 2009 Download for free at http://cnx.org/content/col10322/1.175
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