Lessons · rotation
Rotational kinematics: the same calculus, angular labels
Regime 1 — the algebra is the calculus, evaluated. Step the algebra, step the calculus, and watch the algebra formula fall out of the integral. SymPy proves the two registers agree.
A flywheel starts from rest and spins up under a constant angular acceleration rad/s² for s. How fast is it turning, and how many revolutions has it made? The rotational kinematics are the straight-line equations with angular symbols — step them and watch the timeless equation fall out of the integrals.
A constant net torque gives a constant angular acceleration. Integrate it once for the angular velocity — exactly as constant linear acceleration integrates to .
check and ; show and fall out
- ✓ Angular velocity is the integral of : . [structural]
- ✓ Angular acceleration is constant: . [structural]
- ✓ The memorized timeless equation falls out. [structural]
- ✓ The average-velocity relation holds. [structural]
Dimensional homogeneity: checked by SymPy (holds).
The rotational kinematics equations are the straight-line ones with angular symbols: , , . They come from the same two integrations of a constant acceleration — the slope of the – line is , and the area under it is . Learn one set, relabel, and you have the other.
Modeling assumptions — author-asserted, disclosed not discharged
- Constant angular acceleration (a constant net torque on a rigid body of fixed moment of inertia).
- Rigid body; angles in radians; the axis of rotation is fixed.
The stacked graph, fully annotated
A static rendering (Matplotlib) at the default parameters — the interactive version is in the Graph tab above.
Formulas used
Hover a formula to preview its reference entry; click to open it in the reference (or the concept graph):
- Position under constant acceleration
Valid when: acceleration is constant
Open in reference →
- Velocity under constant acceleration
Valid when: acceleration is constant
Open in reference →