Polar Rose: Polar Coordinates and Curves
Forget left-and-up. Give a distance from the center and a turn of the compass, and curves that look impossible in x and y unfold into flowers and spirals.
A different address system
Cartesian coordinates give directions like a city grid: go x blocks east, then y blocks north. Polar coordinates give directions like a radar operator: turn to angle θ, then walk out a distance r.
The point (r, θ) sits a distance r from the origin (called the pole), along the ray that makes angle θ with the positive x-axis. Every point in the plane has such an address — and for curves built out of rotation, this address is far more natural.
- \( x = r\cos\theta = 2\cos\frac{\pi}{3} = 2\cdot\frac{1}{2} = 1 \).
- \( y = r\sin\theta = 2\sin\frac{\pi}{3} = 2\cdot\frac{\sqrt{3}}{2} = \sqrt{3} \).
Curves as distance rules
A polar curve is written r = f(θ): it tells you, for each direction θ, how far out to place the point. Sweep θ from 0 all the way around and the moving point traces the curve.
Some rules are strikingly simple. r = a is a circle of radius a — the distance never changes as you turn. r = aθ reaches farther the more you turn, spiraling outward (an Archimedean spiral).
Counting the petals
The petal count follows a clean rule that depends on whether k is odd or even. When k is odd, the rose has exactly k petals — the second half of the sweep retraces the first. When k is even, the rose has 2k petals — nothing overlaps, so you get twice as many.
- For r = cos(3θ), k = 3 is odd, so the petal count equals k.
- For r = cos(4θ), k = 4 is even, so the petal count equals 2k = 2(4).
Check your understanding
- Polar coordinates (r, θ) locate a point by distance from the pole and direction, instead of by x and y.
- Convert with x = r cosθ, y = r sinθ, and back with r = √(x²+y²), tanθ = y/x.
- A polar curve r = f(θ) is a distance rule swept around the pole: r = a is a circle, r = aθ is a spiral.
- Rose curves r = a cos(kθ) have k petals when k is odd and 2k petals when k is even.
- Polar coordinates are not unique: adding 2π to θ or using a negative r can name the same point.