When we require only one co-ordinate axis along with time to describe the motion of a particle it is said to be in linear motion or rectilinear motion. Some examples of linear motion are a parade of soldiers, a train moving along a straight line and many more.
Average Velocity
Vav = Total displacement/Total time taken = (rf – ri)/∆t
Instantaneous Velocity (at an instant)
Average acceleration (at an interval)
Instantaneous Acceleration (at an instant)
v is the velocity and t is the time
Equation of motion for constant acceleration
- v=u + at
- s= ut + ½ at2
- v2 = u2 + 2as
- s = {(u+v)/2}t
For a freely falling bodies (u=0)
- v =-gt
- s= -½ gt2
- v2 = – 2gs
- sn = -g/2(2n-1)
Here,
v = final velocity
u = initial velocity
a = acceleration
t = time taken
s = displacement
Graph in Uniformly accelerated Motion along a straight line (a≠0)
- x is a quadratic polynomial in terms of t. Hence x-t graph is a parabola
- v is a linear polynomial in terms of t. Hence v-t graph is a straight line
- a-t graph is a horizontal line because a is a constant
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