Derive the three equations of motion.
The first equation of motion can be derived using a velocity-time graph for a moving object with an initial velocity of u, final velocity v, and acceleration a.
In the above graph,
The velocity of the body changes from A to B in time t at a uniform rate.
BC is the final velocity and OC is the total time t.
A perpendicular is drawn from B to OC, a parallel line is drawn from A to D, and another perpendicular is drawn from B to OE (represented by dotted lines).
Following details are obtained from the graph above:
The initial velocity of the body, u = OA
The final velocity of the body, v = BC
From the graph, we know that BC = BD + DC
Therefore, v = BD + DC
v = BD + OA (since DC = OA)
Finally, v = BD + u (since OA = u) ...........(Equation 1)
Now, since the slope of a velocity-time graph is equal to acceleration a,
So, a = slope of line AB
a = BD/AD
Since AD = AC = t, the above equation becomes:
BD = at ..........(Equation 2)
Now, combining Equation 1 & 2, the following is obtained:
v = u + at
Derivation of Second Equation of Motion by Graphical Method
From the graph above, we can say that
Distance travelled (s) = Area of figure OABC = Area of rectangle OADC + Area of triangle ABD
s=(12AB×BD)+(OA×OC)
Since BD = EA, the above equation becomes
s=(12AB×EA)+(u×t)
As EA = at, the equation becomes
s=12×at×t+(u×t)
On further simplification, the equation becomes
s=ut+12at2.
Derivation of Third Equation of Motion by Graphical Method
From the graph, we can say that
The total distance travelled, s is given by the Area of trapezium OABC.
Hence,
s=12(Sumofparallelsides)×(Height)
s=12(OA+CB)×(OC)
Since, OA = u, CB = v, and OC = t
The above equation becomes
s=12(u+v)×t
Now, since t = (v – u)/a
The above equation can be written as:
s=12(u+v)×(v−u)a
Rearranging the equation, we get
s=v2−u22a