Rotational motion is divided into two parts – (1) pure rotational motion (rotation about a fixed axis), (2) combined translational and rotational motion (CTRM). In this article, we will study the kinematics of rotational motion about a fixed axis. Are you ready to master this topic for the IIT-JEE exam?
As you know, rotational motion is similar to translational (linear) motion in many aspects. Even the terms we use in rotational motion are analogous to the terms used in translational motion. Before we discuss in detail the kinematics of rotation about a fixed axis, let’s quickly peek through the following definitions.
Translational motion involves five primary variables – position, initial velocity, final velocity, acceleration, and time. And each linear variable has a corresponding rotational variable. The parameters of rotational motion are defined as follows.
It is the angle at which a particle rotates around a specified axis. θ (theta) is measured in radians.
It is the rate of change of angular distance (θ) with respect to time. ω is measured in radians per second.
It is the rate of change of angular velocity (ω) with respect to time. α is measured in radians per second squared.
Time is time, irrespective of whether the particle is showing translational motion or rotational motion.
Let’s suppose a particle is undergoing rotational motion about a fixed axis. The particle moves from one point to another, such that the angular displacement is θ.
By definition, angular velocity (ω) is the rate of change of angular displacement. So, mathematically,
ω = dθ/dt
and, similarly,
Angular acceleration α = dω/dt
Since rotational motion parameters are analogous to linear motion variables, rotational motion equations will be similar to kinematical equations for linear motion.
Let’s recall equations for linear motion with constant acceleration.
v = v0+ at
x = x0 + v0t + (1/2) at²
v² = v02+ 2a (x – x0)
where, x0 is the initial displacement, v0 is the initial velocity, x and v are the displacement and velocity of the particle at any given time respectively, a is the acceleration, and t is the time.
The corresponding kinematic equations for rotational motion will be –
ω = ω0+ αt
θ = θ0 + ω0t + (1/2) αt²
ω² = ω02+ 2α (θ – θ0)
Angular displacement θ = x/r
Angular velocity ω = v/r
Angular acceleration α = a/r
Average angular velocity ωavg = (ω0 + ω)/2
No. of rotations of a particle at any given time N = θ/2π
where x, v, a are linear motion parameters, and r is the radius of curvature of the circular path.
Linear (Translational) Motion | Rotational Motion |
v = v0+ at | ω = ω0+ αt |
x = x0 + v0t + (1/2) at² | θ = θ0 + ω0t + (1/2) αt² |
v² = v02+ 2a (x – x0) | ω² = ω02+ 2α (θ – θ0) |
Some common rotational motion examples include rotation of the earth around its axis, blender, drilling machine, the motion of a spinning top, wheels of the motorcycle, merry-go-round, and more.
Solution (a):
α = – 4.0 rad/s2
ω0 = 440 rad/s
ω = 0
θ =?
Using this rotational kinematics equation: ω² = ω02+ 2αθ, we get,
0 = (440)2 + 2(- 4)(θ)
=> θ = 24200 rad = 2.42 x 104 rad
Solution (b):
α = – 4.0 rad/s2
ω0 = 440 rad/s
ω = 0
t =?
Using ω = ω0+ αt, we get
0 = 440 + (- 4) t
=> t = 110s
We know that
ω = 2πf
=> ω = [2π(40)]/60 rad/s = 4.19 rad/s
Solving questions related to rotational motion kinematics is easy. Here are a few pointers that may be of great help while solving numerical problems.
In a nutshell, kinematics is the description of motion. If you know translational motion, the rotational motion will be a piece of cake for you. All you have to do is substitute all the translational motion parameters with rotational motion variables. You can read more articles on translation motion on the Unacademy website.
So far, we have learned about the relationship between various rotational parameters, the analogous relationship between translational and rotational motion, and strategies to solve rotational kinematics problems. Below are a few more questions that may help you with the topic.