Polar Functions

Converting Between Coordinate Systems

Cartesian to Polar

    \(r = \sqrt{x^2 + y^2}\)

    \(\theta = \tan^{-1}(\frac{y}{x})\) with quadrant adjustments:

      Quadrant I: Use \(\theta\) as calculated

      Quadrant II: Add \(\pi\) to \(\theta\)

      Quadrant III: Add \(\pi\) to \(\theta\)

      Quadrant IV: Add \(2\pi\) to \(\theta\)

Polar to Cartesian

    \(x = r\cos(\theta)\)

    \(y = r\sin(\theta)\)

    Remember: Multiple polar coordinates can represent the same point

    If \((r,\theta)\) represents a point, then \((-r,\theta + \pi)\) represents the same point

Common Polar Curves

1. Circle

A circle can be represented in several ways:

    \(r = a\) (circle centered at origin with radius a)

    \(r = 2a\cos(\theta)\) (circle through origin, center at (a,0))

    \(r = 2a\sin(\theta)\) (circle through origin, center at (0,a))

2. Cardioid

A cardioid is a heart-shaped curve given by \(r = a(1 \pm \cos(\theta))\) or \(r = a(1 \pm \sin(\theta))\)

3. Rose Curves

Rose curves are given by \(r = a\cos(n\theta)\) or \(r = a\sin(n\theta)\)

    If n is odd, the curve has n petals

    If n is even, the curve has 2n petals

4. Limaçons

Limaçons have the general form \(r = a \pm b\cos(\theta)\) or \(r = a \pm b\sin(\theta)\)

    If a > b: convex curve

    If a = b: cardioid (special case)

    If a < b: curve with inner loop

Solving Polar Equations

Method 1: Direct Substitution

    Substitute given θ values directly into the equation

    Solve for r

    Check for extraneous solutions

Method 2: Convert to Cartesian Form

    Replace r with \(\sqrt{x^2 + y^2}\)

    Replace \(\cos(\theta)\) with \(\frac{x}{\sqrt{x^2 + y^2}}\)

    Replace \(\sin(\theta)\) with \(\frac{y}{\sqrt{x^2 + y^2}}\)

    Solve the resulting Cartesian equation

    Convert solutions back to polar form if needed

Method 3: Factoring and Algebraic Manipulation

    Group terms with r

    Factor when possible

    Use trigonometric identities to simplify

    Consider domain restrictions:

      r can be negative

      θ typically restricted to [0, 2π) or [-π, π)

      Check for periodicity in θ

Example Problems

1. Solve r = 2cos(θ)

    This is a circle through the origin

    Center at (1,0), radius = 1

    θ ranges from -π/2 to π/2

2. Solve r = 2 + 2cos(θ)

    This is a limaçon

    r is always positive (2 + 2cos(θ) ≥ 0)

    Maximum r = 4 at θ = 0

    Minimum r = 0 at θ = π

Practice Problems

Test your understanding of polar functions and coordinate conversions.