Dynamics Of Rotational Motion : A rigid body is defined as an object that has fixed size and shape. In other words, the relative positions of its constituent particles remain constant. In actual, a rigid body does not exist – it is a useful idealization. By the term fixed axis , we mean that the axis must be fixed relative to the body and fixed in direction relative to an inertial position.
A rigid body may have either of the following three types of motions :
(i) Translational motion
(ii) Rotational motion
(iii) Translational plus rotational motion
A rigid body may have either of the following three types of motions :
(i) Translational motion
(ii) Rotational motion
(iii) Translational plus rotational motion
Motion of body involving rotation can be classified into the following two categories.
(i) Rotation about a fixed axis or pure rotation.
(ii) Rotation about an axis in translation or combined rotation and translation
When a rigid object rotates, points on the object, such as A , B , or C . move in circular paths. An imaginary line perpendicular to plane of circular paths of particles of a rigid body in rotation and containing the centers of all these circular paths is known as axis of rotation. Rotation of ceiling fan, potter's wheel, opening and closing of doors and hands of a wall clock etc. come into this category.
Combined Rotation And Translation : The most general motion of a rigid body is the combination of translational and rotational motions. We have studied pure rotation and pure translation motions but what happens when the two are combined? The most familiar example of combined rotational and translational motion is a rolling wheel. Consider rolling of wheels of a vehicle, moving on straight level road. Relative to a reference frame the axel fixed with the vehicle, the wheel appears rotating about its axel. The rotation of the wheel from this frame is pure rotation about fixed axis. But relative to a reference frame fixed with the ground, the wheel appears rotating about the moving axel, therefore, rolling of a wheel is superposition of two simultaneous but distinct motions-rotation about the fixed axel and translation of the wheel along the level road.
When a body is rotating about a fixed axis, any point P located in the body travels along a circular path. Before, analyzing the circular motion of point P , we will first study the angular motion properties of a rigid body.
Angular Motion : Since, a point is without dimension, it has no angular motion. Only lines or bodies undergo angular motion. Let us consider the angular motion of a radial line r located with the shaded plane.
Angular Position : ∙ The angular position of r is defined by the angle θ, measured between a fixed reference line OA and r .
Angular Displacement : The change in the angular position, often measured as a differential d θ is called the angular displacement. (Finite angular displacements are not vector quantities, although differential rotations d θ are vectors). This vector has a magnitude d θ and the direction of d θ is along the axis.
Angular Velocity :
The time rate of change in the angular position is called the angular velocity
. Thus,
It is expressed here in scalar form, since its direction is always along the axis of rotation, i.e., in the same direction as
Angular Acceleration : ∙ The angular acceleration α measures the time rate of change of the angular velocity. Hence, the magnitude of this vector may be written as,
Thus, for a rigid body we have the rotational analog of Newton’s second law:
…(iii)
Following two points are important regarding the above equations:
(i)
The above equation is valid only for rigid bodies. If the body is not rigid like a rotating tank of water, the angular acceleration
is different for different particles.
(ii)
The sum
in the above equation includes only the torques of the external forces, because all the internal torques add to zero.
Table given ahead compares the linear and angular motion with constant acceleration.
Straight line motion with constant linear acceleration |
Fixed axis rotation with constant angular acceleration |
a = constant |
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v = u + at |
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