Formula and Method for the Cycloid Calculator
A cycloid is the curve traced by a single fixed point on the rim of a circle of radius r as that circle rolls, without slipping, along a straight line. As the circle turns through an angle θ (measured in radians), its center advances horizontally by rθ while the rim point sweeps around the center. Combining that translation with the point's rotation gives the parametric equations x(θ) = r(θ − sin θ) and y(θ) = r(1 − cos θ). This calculator uses those equations to find the traced point's position, plus the classic arc-length and area results for a full arch.
How the calculation works
Enter the radius of the rolling circle and its unit, then a roll angle θ between 0° and 360°. The calculator converts θ to radians and plugs it into x(θ) = r(θ − sin θ) and y(θ) = r(1 − cos θ) to locate the traced point. One complete arch corresponds to θ running from 0 to 2π (360°): its arc length is L = 8r and the area enclosed between the arch and the line is A = 3πr² — both derived by integrating the parametric equations over a full revolution. The arch's height is constant at h = 2r, reached at θ = 180° (the top of the arch). If you set "Number of Arches" above 1, the arc length and area scale linearly, matching a chain of identical arches laid end to end (the pattern traced by a wheel rolling repeatedly).
Common mistakes
- Angle units: the calculator takes θ in degrees and converts internally — do not enter radians directly, or the point position will be wrong.
- Confusing radius with diameter: r in the formulas is the radius of the rolling circle, not its diameter; the arch height (2r) equals the diameter, which can cause mix-ups.
- Arc length vs. base width: the arc length of one arch (8r) is longer than the arch's horizontal base (2πr ≈ 6.28r) because the curve bows upward between the two.
Real-world applications
- Cycloidal gear teeth and pin-wheel (cycloidal) gear profiles use the same rolling-circle geometry to minimize friction and wear.
- The cycloid is the solution to the brachistochrone problem — the shape of a frictionless wire that lets a bead slide between two points in the least time.
- It also solves the tautochrone problem: a ball released from any point on an inverted cycloid reaches the bottom in the same amount of time.
- Cycloidal drives are used in robotics and precision gearboxes for high-ratio, low-backlash speed reduction.