In this tutorial we derive and illustrate the fundamentals of a disc undergoing uniformly accelerated rotation about a fixed axis. We’ll look at kinematic relations, the role of torque, and how to compute the moment of inertia step by step.
When a disc experiences a constant angular acceleration α (rad/s²), its angular velocity ω increases linearly over time:
alpha = d(omega}/dt
For a small time increment dt, the additional angular displacement dφ is
Implementing the motion numerically, at each step we update:
This mirrors the translational kinematic formula s = s + v₀·t + ½·a·t².
To produce angular acceleration, a torque must act on the disc. Torque about the rotation axis is given by
M = F_t * r (N·m)
where Ft is the tangential component of the force at radius r.
The rotational analogue of mass in linear motion is the moment of inertia I. For a rigid body made up of point masses mi at radii ri:
Summing over all mass elements gives the total I, in units of kg·m².
For a uniform solid disc of mass m and radius r, the closed-form result is
Newton’s second law for rotation relates torque and angular acceleration:
The angular momentum L of the rotating disc is