The Acceleration of a Freely Falling Body

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The Acceleration of a Freely Falling Body 

To study the motion of a freely falling body, an object is allowed to fall and its position after successive equal time intervals is recorded on wax-coated paper by means of electric sparks. From these data, graphs of distance vs. time and velocity vs. time are plotted. The acceleration due to gravity is found by determining the slope of the velocity vs. time graph. 

Theory 

In one dimension, an object's average velocity over an interval is the quotient of the distance it travels and the time required to travel that distance:

(1)

where and . The instantaneous velocity at a point is defined as the limit of this ratio as the time interval is made vanishingly small:

(2)

Hence, the velocity is given by the slope of the tangent to the distance vs. time curve. If the velocity were constant the slope would be constant, and the curve would be a straight line. This is evidently not the case for a freely falling body, since it is at rest initially but has nonzero velocities at later times. 

When the velocity of a body varies, the motion is said to be accelerated. The average acceleration over an interval is the quotient of the change of the instantaneous velocity and the time required for that change: 

where . The instantaneous acceleration is defined analogously to the instantaneous velocity: 

(3)

If a body moves in a straight line and makes equal changes of velocity in equal intervals of time, the body is said to exhibit uniformly accelerated motion. This type of motion is produced when the net force upon a body is constant. An example of this is the motion of a body falling freely in a vacuum. The acceleration of the body is called the acceleration due to gravity, g, and has the approximate value of 9.81 m/s2 (= 981 cm/s2 = 32.2 ft/s2) near the surface of the earth. 

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For uniformly accelerated motion (a = constant), the instantaneous acceleration is given by (3), which can be rearranged to give 

When this equation is integrated from time to to t where the respective velocities are vo and v, the result is

(4)

or 

The graph of velocity vs. time is thus a straight line, the slope of which is the acceleration, a. In the experiment the value of g will be determined using this fact. 

When (4) is substituted into (2) and the resulting equation is rearranged, the result becomes 

The value of this expression when integrated from to to ...

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