Study Guide875 words

Double Integrals in Polar Coordinates

Double Integrals in Polar Coordinates

Double Integrals in Polar Coordinates

This guide covers the techniques for evaluating double integrals by transforming Cartesian coordinates (x,y)(x, y) into polar coordinates (r,θ)(r, \theta). This method is particularly powerful for regions with circular symmetry.

Learning Objectives

  • Recognize regions and integrands that are simplified by polar conversion.
  • Apply the transformation dA=rdrdθdA = r \, dr \, d\theta correctly in iterated integrals.
  • Evaluate double integrals over polar rectangular and general polar regions.
  • Convert limits of integration from rectangular to polar form.

Key Terms & Glossary

  • Polar Rectangle: A region RR defined by arba \le r \le b and \alpha \le \theta \le eta.
    • Example: A semi-annulus (half-donut shape) where $1 \le r \le 2and$0θπ and $0 \le \theta \le \pi.
  • Area Element (dAdA): The infinitesimal area dxdydx \, dy which transforms to rdrdθr \, dr \, d\theta in polar coordinates.
    • Example: When integrating over a disk, the "extra rr" accounts for the widening of sectors as rr increases.
  • General Polar Region: A region bounded by two rays (θ=α,θ=β\theta = \alpha, \theta = \beta) and two continuous functions of θ\theta (r=h1(θ),r=h2(θ)r = h_1(\theta), r = h_2(\theta)).
    • Example: The interior of a cardioid r=1+cos(θ)r = 1 + \cos(\theta).

The "Big Idea"

In Cartesian coordinates, circular boundaries result in integration limits involving square roots (e.g., y=a2x2y = \sqrt{a^2 - x^2}), which are often difficult to compute. By switching to polar coordinates, circular boundaries become constant limits (r=ar = a), turning complex regions into "rectangles" in the rθr\theta-plane. This effectively "straightens out" the geometry of the problem.

Formula / Concept Box

Transformation RuleCartesian to Polar
Coordinate Substitutionx=rcosθx = r \cos \theta, y=rsinθy = r \sin \theta
Radius Relationshipr2=x2+y2r^2 = x^2 + y^2
Area ElementdA=rdrdθdA = r \, dr \, d\theta
Double Integral FormRf(x,y)dA=αβh1(θ)h2(θ)f(rcosθ,rsinθ)rdrdθ\iint_R f(x,y) \, dA = \int_{\alpha}^{\beta} \int_{h_1(\theta)}^{h_2(\theta)} f(r \cos \theta, r \sin \theta) \, r \, dr \, d\theta

[!IMPORTANT] Never forget the extra rr in the integrand! dxdydrdθdx \, dy \neq dr \, d\theta. The correct substitution is dxdy=rdrdθdx \, dy = r \, dr \, d\theta.

Hierarchical Outline

  • I. Motivation for Polar Integration
    • Circular Symmetry: Use when the region DD is a disk, ring, or sector.
    • Integrand Simplification: Use when f(x,y)f(x,y) contains the term x2+y2x^2 + y^2.
  • II. Integration over Polar Rectangles
    • Constant Limits: Bounds are arba \le r \le b and αθβ\alpha \le \theta \le \beta.
    • Iterated Setup: Outer integral usually θ\theta, inner integral rr.
  • III. Integration over General Polar Regions
    • Functional Limits: rr varies between two polar curves r=g(heta)r = g( heta) and r=h(heta)r = h( heta).
    • Radial Arrows: Visualize by drawing a ray from the origin through the region.

Visual Anchors

Decision Flow: When to use Polar Coordinates?

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Figure 1 — Mermaid diagram

Geometry of the Polar Area Element

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Figure 2 — TikZ diagram

Definition-Example Pairs

  • Definition: Annular Region — The area between two concentric circles.
    • Real-World Example: Finding the mass of a circular metal washer with a hole in the center. The density might vary with distance from the center.
  • Definition: Radial Bound — The function r(θ)r(\theta) that defines the outer edge of a shape.
    • Real-World Example: A lighthouse beam rotating; the area swept over a specific time is a sector defined by the range of the beam (rr) and the angle of rotation (θ\theta).

Worked Examples

Example 1: Evaluating over a Disk

Evaluate Dex2+y2dA\iint_D e^{x^2+y^2} \, dA where DD is the unit disk x2+y21x^2 + y^2 \le 1.

  1. Convert Region: The unit disk is $0 \le r \le 1and$0θ2π and $0 \le \theta \le 2\pi.
  2. Convert Integrand: ex2+y2er2e^{x^2+y^2} \rightarrow e^{r^2}.
  3. Setup Integral: 02π01er2(rdrdθ)\int_0^{2\pi} \int_0^1 e^{r^2} (r \, dr \, d\theta)
  4. Evaluate Inner (rr): Let u=r2,du=2rdru = r^2, du = 2r \, dr. 01rer2dr=[12er2]01=12(e1)\int_0^1 r e^{r^2} \, dr = \left[ \frac{1}{2} e^{r^2} \right]_0^1 = \frac{1}{2}(e - 1)
  5. Evaluate Outer (θ\theta): 02π12(e1)dθ=12(e1)[2π]=π(e1)\int_0^{2\pi} \frac{1}{2}(e - 1) \, d\theta = \frac{1}{2}(e - 1) [2\pi] = \pi(e - 1)

Example 2: General Polar Region

Find the area of the region DD inside the cardioid r=1+cosθr = 1 + \cos \theta.

  1. Setup: Area A=D1dA=02π01+cosθrdrdθA = \iint_D 1 \, dA = \int_0^{2\pi} \int_0^{1+\cos \theta} r \, dr \, d\theta.
  2. Inner Integral: 01+cosθrdr=[12r2]01+cosθ=12(1+cosθ)2=12(1+2cosθ+cos2θ)\int_0^{1+\cos \theta} r \, dr = \left[ \frac{1}{2} r^2 \right]_0^{1+\cos \theta} = \frac{1}{2}(1 + \cos \theta)^2 = \frac{1}{2}(1 + 2\cos \theta + \cos^2 \theta)
  3. Use Identity: cos2θ=1+cos2θ2\cos^2 \theta = \frac{1 + \cos 2\theta}{2}.
  4. Outer Integral: 02π12(1+2cosθ+12+12cos2θ)dθ=12[32θ+2sinθ+14sin2θ]02π=3π2\int_0^{2\pi} \frac{1}{2} (1 + 2\cos \theta + \frac{1}{2} + \frac{1}{2}\cos 2\theta) \, d\theta = \frac{1}{2} [ \frac{3}{2}\theta + 2\sin \theta + \frac{1}{4}\sin 2\theta ]_0^{2\pi} = \frac{3\pi}{2}

Checkpoint Questions

  1. What is the Jacobian (the scaling factor) when moving from Cartesian to Polar double integrals?
  2. If you are integrating over a region in the first quadrant bounded by y=xy=x, y=0y=0, and x2+y2=9x^2+y^2=9, what are the θ\theta limits?
  3. True or False: 0101f(r,θ)drdθ\int_0^1 \int_0^1 f(r, \theta) \, dr \, d\theta represents the integral over a square of side length 1 in the xyxy-plane.
Click to see answers
  1. The factor is rr.
  2. θ\theta goes from 0 to π/4\pi/4.
  3. False. It represents a unit sector (a quarter-circle with radius 1).

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