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Arranging terms with same variable on one side of the equation, we have :

đ x = v đ v a v

Integrating, we have :

Δ x = v đ v a v

Evaluation of this relation results an expression of velocity in x. Clearly, we can proceed as before to obtain expression of position in t.

Problem : The motion of a body in one dimension is given by the equation dv(t)/dt = 6.0 -3 v (t), where v(t) is the velocity in m/s and “t” in seconds. If the body was at rest at t = 0, then find the expression of velocity.

Solution : Here, acceleration is given as a function in velocity as independent variable. We are required to find expression of velocity in time. Using integration result obtained earlier for expression of time :

Δ t = đ v a v

Substituting expression of acceleration and integrating between t=0 and t=t, we have :

Δ t = t = đ v ( t ) 6 - 3 v ( t )

t = ln [ { 6 - 3 v ( t ) 6 ] - 3

6 - 3 v ( t ) = 6 e - 3 t 3 v ( t ) = 6 ( 1 - e - 3 t ) v ( t ) = 2 ( 1 - e - 3 t )

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Graphical method

We analyze graphs of motion in parts keeping in mind regular geometric shapes involved in the graphical representation. Here, we shall work with two examples. One depicts variation of velocity with respect to time. Other depicts variation of acceleration with respect to time.

Velocity .vs. time

Problem : A particle moving in a straight line is subjected to accelerations as given in the figure below :

Acceleration – time plot

Acceleration – time plot

If v = 0 and t = 0, then draw velocity – time plot for the same time interval.

Solution : In the time interval between t = 0 and t = 2 s, acceleration is constant and is equal to 2 m / s 2 . Hence, applying equation of motion for final velocity, we have :

v = u + a t

But, u = 0 and a = 2 m / s 2 .

v = 2 t

The velocity at the end of 2 seconds is 4 m/s. Since acceleration is constant, the velocity – time plot for the interval is a straight line. On the other hand, the acceleration is zero in the time interval between t = 2 and t = 4 s. Hence, velocity remains constant in this time interval. For time interval t = 4 and 6 s, acceleration is - 4 m / s 2 .

From the plot it is clear that the velocity at t = 4 s is equal to the velocity at t = 2 s, which is given by :

u = 2 x 2 = 4 m / s

Velocity – time plot

Corresponding velocity – time plot.

Putting this value as initial velocity in the equation of velocity, we have :

v = 4 - 4 t

We should, however, be careful in drawing velocity plot for t = 4 s to t = 6 s. We should relaize that the equation above is valid in the time interval considered. The time t = 4 s from the beginning corresponds to t = 0 s and t = 6 s corresponds to t = 2 s for this equation.

Velocity at t = 5 s is obtained by putting t = 1 s in the equation,

v = 4 - 4 x 1 = 0

Velocity at t = 6 s is obtained by putting t = 2 s in the equation,

v = 4 - 4 x 2 = - 4 m / s

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Acceleration .vs. time

Problem : A particle starting from rest and undergoes a rectilinear motion with acceleration “a”. The variation of “a” with time “t” is shown in the figure. Find the maximum velocity attained by the particle during the motion.

Acceleration – time plot

The area under plot gives change in velocity.

Solution : We see here that the particle begins from rest and is continuously accelerated in one direction (acceleration is always positive through out the motion) at a diminishing rate. Note that though acceleration is decreasing, but remains positive for the motion. It means that the particle attains maximum velocity at the end of motion i.e. at t = 12 s.

The area under the plot on acceleration – time graph gives change in velocity. Since the plot start at t = 0 i.e. the beginning of the motion, the areas under the plot gives the velocity at the end of motion,

Δ v = v 2 - v 1 = v - 0 = v = 1 2 x 8 x 12 = 48 m / s

v max = 48 m / s

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Source:  OpenStax, Physics for k-12. OpenStax CNX. Sep 07, 2009 Download for free at http://cnx.org/content/col10322/1.175
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