Introduction of Motion
Motion means change in position of an object with respect to its surroundings in a given interval of time. We see various things around us in motion, e.g. water flowing in a river, flowers nodding to blowing wind, birds flying in the sky, a player running in the playground and many more. Motion is a relative phenomenon, i.e., an object appearing to be in motion to one person can appear to be at rest to another person, e.g. to a person driving a car, trees on roadside might appear to move backward while same tree will appear to be at rest to a person standing on roadside.
Describing Motion
Two different physical quantities the distance and the displacement, are used to describe the overall motion of an object and to locate its final position with reference to its initial position at a given time. Since motion is a relative concept, we need a reference point to describe the position of an object. We call this reference point as origin.
Consider an object moving in a straight line. Let the object starts from a point O. This starting point o is taken as the reference point. After 10 minutes, it reaches the position P3 through P, and P2
(time taken from O to reach P3= 10 min)
(ii) If distance-time graph of an object is a straight line parallel to the time axis, as shown in graph, we say the position of the object does not change with time, or the object remains at rest. Here slope of line is Zero hence velocity is zero,
(iii) If we get a curved line in distance-time graph, if we find that slope for any two time intervals, will not be same. Or we say the object has a non-uniform speed, i.e. the body is accelerated. Slope at point P is more than that at point Q. Hence velocity increases with time.
Displacement-Time Graph
We know that displacement of an object can be negative also, while distance is always positive. Thus, displacement-time graph differs from distance-time graph in the following manner: First, when the object moves with a uniform velocity, it is given by
the slope of line OA. Velocity =AP/OP
After that, object moves with a constant velocity which is given by the slope of line AB.
Now, slope of line AB =SB-SA/tB-tA
= 0-6/6-3
= -6/3
= -2
It is negative.
We say, the object moves with velocity -2 m/s. i.e. with a velocity 2 m/s in opposite direction. It comes to original position in 6 sec (net Time (s)displacement zero) and then moves to the other side maintaining its velocity
Velocity-Time Graph
In this graph, variation of velocity of an object with time is shown. Time is taken along x-axis while velocity is taken along y-axis.
- For uniformly accelerated motion
Consider the velocity-time graph shown. It is a straight line with a positive slope passing through the origin. Consider any two positions A and B of the object, at instants tī and t2 when the object has velocities u and v respectively.
Now according to definition of acceleration,
a=∆v/∆t=v-u/t²-t¹ eq (1st)
=AC/BC= slope of the straight line
Thus, slope of the graph obtained in a velocity time graph gives the acceleration of the object. Now for a straight line, the slope will be same for any two points considered. Or we can say that acceleration will remain constant or uniform.
Thus, a uniformly accelerated motion is shown by a straight line having a positive slope in a
time graph.
Consider equation (i),
a=v-u/t²-t¹
Let t² - t¹=t
=> a=v-u/t
v=u + at
which is one of the very important equations of motion.
For a uniform motion : When an object is in uniform motion, it will have a constant velocity at every instant. i.e. velocity won't change with time or we can say that velocity-time graph is a straight line parallel to time-axis.
Now acceleration between any two instants t1, and t2 is
a=Δυ/∆t=v-v/t²-t¹= 0
Velocity (m/s)
Thus, acceleration is zero for an object having uniform motion. Also according to the definition of velocity,
total displacement
Average velocity=total displacement/total time taken
Again taking same time interval between two instants t¹and to t²
v=S/t²-t¹
=s=v x (t2 - +t¹) = AB× BC
= Area of the shaded region shown in adjacent graph.
Thus distances of the object is given by the area enclosed by velocity-time graph and the time axis. Distance can also be obtained for a uniformly accelerated motion using the same method.
For example: Total distance = area of trapezium ABEDA
s = Area of rectangle BCDE + Area of triangle ABC.
= BE× ED +{½×AC×BC =u× (t² – t¹)+(½v–u)×(t²– t)
Let time interval t²-t¹=t
s=ut +½(v-u) t
Using equation, v=u + at, we get
=> S=ut +½(at)t
S=ut +½at²
This is second equation of motion.
Consider the figure given above once again,
s = Area of trapezium ABEDA =½×ED(BE + AD)
=½t(u + v) ½(v-u/a (v+u)
= ½a(v²-u²) or
=>V²-u²=2aS
- For uniformly retarded motion :
For this, velocity-time graph is a straight line having a negative slope.
- For non-uniformly accelerated motion :
For this, velocity-time graph can have any shape depending upon how the velocity varies. Here, acceleration will be different between different instants as the slope does not remain constant. The graphs discussed above can also be used to make a comparative study of motion of two or more objects. Consider the illustration given.
Uniform Circular Motion
If an object moves in a circular path with uniform speed, its motion is called uniform circular motion.
A circular path can be made up of an indefinite number of small sides, and a body moving along such a circular path changes its direction of motion continuously. Therefore, if you run on a circular track, you change your direction infinite times in one round. Four arbitrary points on the circular path and the direction of motion of the body at these points are shown. Since the direction of motion changes, uniform circular motion is a case of accelerated motion. Direction of acceleration is always towards centre and its magnitude is v2/r at all points
Note: If a body moves on a circular path of radius r and completes one rotation in time t, then the distance
covered by the body is equal to the circumference of the circle, i.e., 2 πr. In such a case speed v is given by, v=2πr/t
Examples of circular motion
- A stone tied to a thread and whirled in a circular path.
- Wheels of various vehicles rotating about their axles.
- A satellite revolving around the Earth in a circular path at constant speed.
- The Moon revolving around the Earth in a circular path at constant speed.
In the above examples, the speed is uniform but the velocity is variable due to continuous change in direction. Thus, the bodies have an accelerated motion.....
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Good going sir
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