Motion
of Body Under Gravity (Free Fall)
The force of attraction of earth on
bodies, is called force of gravity. Acceleration produced in the body by the
force of gravity, is called acceleration due to gravity. It is represented by
the symbol g.
In the absence of air resistance, it is found that all bodies
(irrespective of the size, weight or composition) fall with the same
acceleration near the surface of the earth. This motion of a body falling
towards the earth from a small altitude (h
<< R) is called free fall.
An ideal example of one-dimensional motion is motion under gravity
in which air resistance and the small changes in acceleration with height are
neglected.
(1) If a body is dropped from some height (initial velocity zero)
(i) Equations of motion : Taking initial position as origin and
direction of motion (i.e., downward
direction) as a positive, here we have
u = 0 [As body starts from
rest]
a = +g [As
acceleration is in the direction of motion]
v = g t …(i)
…(ii)
…(iii)
...(iv)
(ii) Graph of distance, velocity and acceleration with respect to
time :
(iii) As h = (1/2)gt2, i.e., h µ t2, distance
covered in time t, 2t, 3t,
etc., will be in the ratio of 12
: 22 : 32, i.e.,
square of integers.
(iv) The distance covered in the nth
sec,
So distance covered in 1st, 2nd, 3rd
sec, etc., will be in the ratio of 1 : 3 : 5, i.e., odd integers only.
(2) If a body is projected
vertically downward with some initial velocity
Equation of motion :
(3) If a body is projected
vertically upward
(i) Equation of motion : Taking initial position as origin and
direction of motion (i.e., vertically
up) as positive
a = – g [As acceleration is
downwards while motion upwards]
So, if the body is projected with velocity u and after time t it
reaches up to height h then
;;;
(ii) For maximum height v
= 0
So from above equation u =
gt,
and
(iii) Graph of displacement, velocity and acceleration with respect
to time (for maximum height) :
It is clear that both quantities do not depend upon the mass of the
body or we can say that in absence of air resistance, all bodies fall on the
surface of the earth with the same rate.
(4) The motion is independent of the mass of the body, as in any
equation of motion, mass is not involved. That is why a heavy and light body
when released from the same height, reach the ground simultaneously and with
same velocity i.e., and .
(5) In case of motion under gravity, time taken to go up is equal to
the time taken to fall down through the same distance. Time of descent (t2) = time of ascent (t1) = u/g
\ Total time of flight T = t1 + t2
(6) In case of motion
under gravity, the speed with which a body is projected up is equal to the
speed with which it comes back to the point of projection.
As well as the magnitude
of velocity at any point on the path is same whether the body is moving in
upwards or downward direction.
(7) A body is thrown vertically upwards. If air resistance is to be
taken into account, then the time of ascent is less than the time of
descent. t2 > t1
Let u is the initial
velocity of body then time of ascent and
where g is acceleration
due to gravity and a is retardation
by air resistance and for upward motion both will work vertically downward.
For downward motion a and g will work in opposite direction
because a always work in direction
opposite to motion and g always work
vertically downward.
So
Þ
Þ
Comparing t1
and t2 we can say that t2 > t1
since (g + a ) > (g – a)
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