Equations of motion by graphical method
Tanusri Gururaj, Academic content writer of Physics at Edumarz
Let us assume that a body moves on a straight line with uniform acceleration. There are certain relations between its velocity, acceleration, and the distance covered by it in a time interval.
These relations are given by the following equations:
v = u + at
s = ut + ½ at2
2as = v2 – u2
v = final velocity
u = initial velocity
t = time
s = distance travelled by the body in the time interval ‘t’
a = uniform acceleration
To obtain the equations of motion, we will use the following graph:
First equation:
The time interval in which the velocity of a body changes from ‘u’ to ‘v’ is OE. The body also has uniform acceleration ‘a.’
Lines CE and CD are drawn perpendicular to the x and y-axis respectively. Line AB is drawn parallel to line OE.
According to the graph,
CE = CB + BE or CE = CB + OA
But, OA = u and CE = v
So, CB = v – u
Also, a = change in velocity of body/time taken
a = CB/t
a = (v – u)/t
On cross-multiplying we get,
v = u + at
Second equation:
Let us consider that the body has travelled a distance ‘s’ in time ‘t’ under uniform acceleration ‘a.’
Distance covered by the object = area under the graph
s = area of triangle ABC + area of rectangle ABEO
Area of triangle = ½ x (base x height)
Area of rectangle = length x breadth
s = ½ x (AB x CB) + OE x BE
s = ½ x (t x at) + t x u
s = ut + ½ at2
Third equation:
The distance covered by the body = area enclosed within the trapezium OACE
Area of trapezium OACE = ½ x (sum of parallel sides) x distance between them
s = ½ x (OA + CE) x OE
s = ½ x (u + v) x t
From the first equation of motion we have
t = (v – u)/a
After substituting t in the third equation of motion we get
s = ½ x (u + v) x (v – u)/a
On solving we get the equation,
2as = v2 – u2