Physics, asked by vijatasharma035, 7 months ago

Drive the Equation of motion by graphical motion.​

Answers

Answered by TSAlva
1

Consider the velocity-time graph of an object

that moves under uniform acceleration as own in Fig. 8.8 (similar to Fig. 8.6, but now

with u ≠ 0). From this graph, you can see that

initial velocity of the object is u (at point A)

and then it increases to v (at point B) in time

t. The velocity changes at a uniform rate a.

In Fig. 8.8, the perpendicular lines BC and

BE are drawn from point B on the time and

the velocity axes respectively, so that the

initial velocity is represented by OA, the final

velocity is represented by BC and the time

interval t is represented by OC. BD = BC –

CD, represents the change in velocity in time

interval t.

Let us draw AD parallel to OC. From the

graph, we observe that

BC = BD + DC = BD + OA

Substituting BC = v and OA = u,

we get v = BD + u

or BD = v – u (8.8)

From the velocity-time graph (Fig. 8.8),

the acceleration of the object is given by

a =

Change in velocity

time taken

= BD BD = AD OC

Substituting OC = t, we get

a = BD

t

or BD = at (8.9)

Using Eqs. (8.8) and (8.9) we get

v = u + at

Let us consider that the object has travelled

a distance s in time t under uniform

acceleration a. In Fig. 8.8, the distance

travelled by the object is obtained by the area

enclosed within OABC under the velocity-time

graph AB.

Thus, the distance s travelled by the object

is given by

s = area OABC (which is a trapezium)

= area of the rectangle OADC + area of

the triangle ABD

= OA × OC +

1

2 (AD × BD) (8.10)

Substituting OA = u, OC = AD = t and BD

= at, we get

s = u × t +

1 ( ) 2

t ×at

or s = u t +

1

2 a t 2

8.5.3 EQUATION FOR POSITION–VELOCITY

RELATION

From the velocity-time graph shown in

Fig. 8.8, the distance s travelled by the object

in time t, moving under uniform acceleration

a is given by the area enclosed within the

trapezium OABC under the graph. That is,

s = area of the trapezium OABC

= OA + BC ×OC

2

Substituting OA = u, BC = v and OC = t,

we get

2

u+v t

s (8.11)

From the velocity-time relation (Eq. 8.6),

we get

v–u

t =

a (8.12)

Using Eqs. (8.11) and (8.12) we have

[v+u] {v-u] s =  2a

or 2 a s = v2 – u2

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