he velocity-time graph for uniformly accelerated rectilinear motion (motion along a straight line), a > 0, is illustrated in the figure.
The velocity-time graph for a uniformly retarded motion is as shown in the figure. Here a < 0, indicating retardation or deceleration.
In this section, we are going to derive the velocity-time relation for a particle moving with constant acceleration.
The figure above illustrates a particle moving with constant acceleration 'a' along the positive direction of X-axis. If v (t1) and v (t2) be the velocities of the particle at times t1 and t2 respectively, then
Acceleration, according to the definition
Cross-multiplying, we have,
v (t2) - v (t1) = a (t2 - t1)
v (t2) = v (t1) + a (t2 - t1)
If the motion is considered from t = 0, then the corresponding velocity v(0) at t = 0 is called the initial velocity and the velocity after a time interval, say t, is called the final velocity and denoted by v(t). In this case, the acceleration is given by
or at = v (t) - v (0)
v(t) = v (0) + at
The above expression represents the first equation of motion.
The figure below illustrates the velocity-time graph AB of a uniformly accelerated particle. The points A and B correspond to velocities v (0) and v (t) respectively.
Slope of the straight line AB
Also, from the definition of acceleration, we know that
We conclude that the slope of the velocity-time graph for uniformly accelerated motion gives the acceleration.At any given time, the direction of motion is given by velocity and not by acceleration. As an example, when a ball is thrown up vertically, its velocity is directed upwards at any given time, but its acceleration is always directed in the downward direction.
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