Question
State the kinematic equations for uniformly accelerated motion.

Answer

For uniformly accelerated motion, we can derive some simple equations that relate displacement(x), time taken(t), Initial velocity(u), final velocity (v) and acceleration(a).

  1. Velocity attained after time t: The velocity-time graph for positive constant acceleration of a particle is shown in the figure.

Let u be the initial velocity of the particle at t = 0 and v is the final velocity of the particle after time t. Consider two points A and B on the curve corresponding to t = 0 and t = t respectively.

Draw BD perpendicular to time axis. Also draw AC perpendicular to BD.

$\therefore$ OA = CD = u;

BC = (v - u) and OD = t

Now slope of v-t graph = acceleration (a)

$\therefore$ a = slope of v-t graph $=\tan\theta=\frac{\text{BC}}{\text{AC}}=\frac{\text{BC}}{\text{OD}}$ [$\because$ AC= OD]

$\therefore \text{a}=\frac{\text{v}-\text{u}}{\text{t}}$

$\text{v}-\text{u}=\text{at}$

 or $\text{v}=\text{u}+\text{at}$

  1. Distance travelled in time t:

Let, x0 = position of the particle at t = 0 from the origin.

x = position of the particle at t = t from the origin.

$\therefore$ (x - x0) = S = distance travelled by the particle in the time interval (t - 0) = t

We know, distance travelled by a particle in the given time

Interval = area under velocity-time graph

$\therefore$ (x – x0) = Area OABD (see fig, above) = Area of trapezium OABD

$=\frac{1}{2}$ [Sum of parallel sides × perpendicular distance between parallel sides]

$=\frac{1}{2}(\text{OA}+\text{BD})\times\text{AC}=\frac{1}{2}(\text{u}+\text{v})\times\text{t}$

Since $\text{v}=\text{u}+\text{at}$

$\therefore(\text{x}-\text{x}_0)=\frac{1}{2}(\text{u}+\text{u}+\text{at})\times\text{t}$

$=\frac{1}{2}(2\text{u}+\text{at})\times\text{t}=\text{ut}+\frac{1}{2}\text{at}^2$

Since $\text{x}-\text{x}_0=\text{S}$

$\therefore \text{S}=\text{ut}+\frac{1}{2}\text{at}^2$

  1. Velocity attained after travelling a distance S: We know, distance travelled by a particle in time t is equal to the area under velocity-time graph. Therefore, the distance (s) travelled by a particle during time interval t is given by

S = Area under v-t graph (see fig.) or

S = area of trapenium OABD

$=\frac{1}{2}$ (sum of parallel sides) × perpendicular distance between these para

$\text{S}=\frac{1}{2}(\text{OA}+\text{BD})\times\text{ACs}\ \dots(\text{i})$

Now, acceleratiory a = slope of v- t graph

$\text{a}=\frac{\text{BC}}{\text{AC}}=\frac{\text{BD}-\text{CD}}{\text{AC}}=\frac{\text{v}-\text{u}}{\text{AC}}$

$\text{AC}=\Big(\frac{\text{v}-\text{u}}{\text{a}}\Big)\text{s}$

Also, OA = u and BD = v

Using equations (ii) and (iii) in equation (i), we get

$\text{S}=\frac{1}{2}(\text{v}+\text{u})\frac{(\text{v}-\text{u})}{\text{a}}=\frac{\text{v}^2-\text{u}^2}{2\text{a}}$

$\text{v}^2-\text{u}^2=2\text{as}$

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