Undergraduate → Classical mechanics ↓
Rotational motion
Rotational motion is a fundamental concept in classical mechanics that describes the motion of objects or systems that rotate around a central axis. While linear motion deals with objects moving along a path in a straight line, rotational motion involves objects that spin or revolve.
Understanding rotational motion is important for analyzing systems ranging from spinning tops and gears to the rotation of planets and stars. Several key concepts and equations describe rotational motion, which are similar to the equations describing linear motion, but with different variables.
Angular displacement, velocity and acceleration
Similar to linear displacement, velocity, and acceleration, rotational motion involves angular displacement, angular velocity, and angular acceleration.
Angular displacement is the angle through which a point or line has been rotated in a specified sense about a specified axis. It is measured in radians.
Δθ = θ_f - θ_i
where Δθ
is the angular displacement, θ_f
is the final angular position, and θ_i
is the initial angular position.
Angular velocity (ω) is the rate at which an object rotates. It is described by the change in angular displacement over time and is measured in radians per second (rad/s).
ω = Δθ / Δt
where ω
is the angular velocity, Δθ
is the angular displacement, and Δt
is the time interval.
Angular acceleration (α) tells how quickly the angular velocity changes with time. It is measured in radians per second squared (rad/s²).
α = Δω / Δt
where α
is the angular acceleration, Δω
is the change in angular velocity, and Δt
is the time interval.
Visualization of rotational motion
Imagine a rotating wheel. The wheel has a central axis and rotates around it. To understand these concepts further, consider the following illustration:
In this representation, the black lines represent the reference and current angular positions of a point on the wheel, and the red line represents the angular displacement, Δθ
.
Equations of rotational motion
The equations describing rotational motion have the same form as the equations of linear motion. However, they use an angular analog.
- Final angular velocity:
ω_f = ω_i + αt
- Angular displacement:
θ = ω_i t + 0.5αt^2
- Square of final angular velocity:
ω_f^2 = ω_i^2 + 2αθ
In these formulas, ω_i
is the initial angular velocity, ω_f
is the final angular velocity, α
is the angular acceleration, and θ
is the angular displacement.
Moment of inertia
Moment of inertia, denoted as I
, is a measure of an object's resistance to a change in its rotational speed. It depends on the mass distribution of the object relative to the axis of rotation.
The simple equation for a point mass is:
I = mr²
Where m
is the mass of the object and r
is the distance of the mass from the axis of rotation.
For more complex objects, the moment of inertia requires summing or integration of all mass elements:
I = Σ(m_i r_i²)
or, for a persistent object:
I = ∫ r² dm
Torque
Torque is the rotational analog of force. It measures how much a force applied to an object rotates it.
τ = r × F
Where τ
is the torque, r
is the position vector from the axis of rotation to the point where the force is applied, and F
is the force vector. The cross product indicates that the torque depends on both the magnitude and direction of the force, as well as the distance from the axis.
Newton's second law for rotational motion
As with linear motion, a form of Newton's second law applies to rotational motion. It states that the net torque acting on an object is equal to the product of its moment of inertia and angular acceleration.
Στ = Iα
Example problems
Let us consider some practical examples of solving rotational motion problems to strengthen our understanding.
Example 1: Spinning disc
A disc of radius 0.5 m and mass 2 kg is initially at rest. A force of 10 N is applied tangentially to its edge. Find the angular acceleration.
First, calculate the moment of inertia of the disc using the formula for a solid disc:
I = 0.5 * m * r²
I = 0.5 * 2 kg * (0.5 m)² = 0.25 kg·m²
Apply the torque formula:
τ = r × F = 0.5 m × 10 N = 5 N·m
Use Newton's second law for rotation:
Στ = Iα => 5 N·m = 0.25 kg·m² * α
α = 5 N·m / 0.25 kg·m² = 20 rad/s²
Example 2: Rotating rod
A thin rod of length 1 m and mass 3 kg is fixed at one end and is free to rotate. A force of 15 N is applied perpendicularly at the centre of the rod. Calculate the angular acceleration.
Calculate the moment of inertia about the pivot at one end:
I = (1/3) * m * L²
I = (1/3) * 3 kg * (1 m)² = 1 kg·m²
Calculate the torque:
τ = r × F = 0.5 m × 15 N = 7.5 N·m
Apply Newton's second law:
Στ = Iα => 7.5 N·m = 1 kg·m² * α
α = 7.5 rad/s²
Conclusion
Rotational motion is important in understanding many physical phenomena and engineering systems. By mastering key concepts such as angular velocity, angular acceleration, torque, and moment of inertia, you can analyze and predict complex rotational behaviors.
Continued exploration of rotational motion will not only enrich the understanding of classical mechanics principles but will also lead to advances in practical applications such as machinery design and astrophysics.