Polar coordinates offer a completely different way to describe position in a plane — using a distance r from the origin and an angle θ (theta) from the positive x-axis. Many beautiful curves that are complicated in Cartesian form become elegantly simple in polar form. Open the graphing calculator to follow this guide.
Understanding Polar Coordinates
In Cartesian coordinates, a point is described by (x, y). In polar coordinates, it's described by (r, θ) where:
- r = the distance from the origin (radius)
- θ = the angle measured counterclockwise from the positive x-axis (in radians)
Conversion between the two systems:
x = r · cos(θ)y = r · sin(θ)r = sqrt(x² + y²)
Enabling Polar Mode
In the graphing calculator, open the Settings panel (gear icon in the toolbar) and enable Polar mode. In polar mode, you enter equations in the form r = f(θ) and the calculator plots the curve parametrically as θ sweeps from 0 to 2π.
Basic Polar Curves
Circle
The simplest polar curve is a circle centred at the origin:
r = 3 — a circle with radius 3
Compare with the Cartesian form: x² + y² = 9. The polar form is much simpler!
Rose Curves
Rose curves have petals determined by the coefficient inside the trig function:
r = cos(2*θ)— 4-petal rose (even n gives 2n petals)r = cos(3*θ)— 3-petal rose (odd n gives n petals)r = sin(4*θ)— 8-petal roser = cos(5*θ)— 5-petal rose
Cardioid
A cardioid is a heart-shaped curve formed when the radius includes both a constant and trig term of equal magnitude:
r = 1 + cos(θ)— cardioid pointing rightr = 1 - sin(θ)— cardioid pointing downr = 2 + 2*cos(θ)— larger cardioid
Limaçon
A limaçon is a generalisation of the cardioid where the constant and trig coefficient differ:
r = 2 + 3*cos(θ)— limaçon with inner loop (if |b| > |a|)r = 3 + 2*cos(θ)— convex limaçon (if |a| > |b|)r = 2 + 2*cos(θ)— cardioid (when |a| = |b|)
💡 Use a slider on the coefficients to smoothly transition between limaçon types: r = a + b*cos(θ) with sliders for a and b.
Spirals
Spirals are curves that wind outward from the origin:
r = θ— Archimedean spiral (evenly spaced coils)r = θ / (2*pi)— 1 unit of radius per full rotationr = exp(0.2*θ)— logarithmic spiral (found in nature)
Lemniscate
A figure-eight shaped curve:
r = sqrt(cos(2*θ))— lemniscate of Bernoulli (only defined where cos(2θ) ≥ 0)r^2 = 4*cos(2*θ)— note: r² form; use r = sqrt(...) to approximate
Converting Between Cartesian and Polar
Some Cartesian equations become much simpler in polar form. For example:
- Circle
x² + y² = 25→r = 5 - Line through origin
y = x→θ = π/4(a ray) - Parabola
y = x²→r·sin(θ) = r²·cos²(θ)→ complex!
Symmetry in Polar Curves
Polar curves can have beautiful symmetry:
- Symmetric about x-axis: if replacing θ with −θ gives the same equation
- Symmetric about y-axis: if replacing θ with π − θ gives the same equation
- Symmetric about origin: if replacing r with −r gives the same equation
Verify: graph r = cos(θ) — you'll see it's symmetric about the x-axis.
- Graph
r = 1 + 2*cos(θ). Does it have an inner loop? At what angle does the loop occur? - Graph
r = cos(6*θ). How many petals does the rose have? - Graph
r = θ(Archimedean spiral). How many full rotations does it make before r = 10? - Use sliders on
r = a + b*cos(θ). At what value of a/b does the inner loop appear/disappear?