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9231 · 1.5

Polar coordinates — practice questions

Practice and worked examples for 9231 Polar coordinates. Short previews only — attempt the full question in MarkScheme against the official scheme.

Worked example 1

Sketch the curve given by the polar equation r=3(1+cos⁡θ)r = 3(1 + \cos\theta) for 0≤θ≤2π0 \le \theta \le 2\pi.

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This is a cardioid. The presence of cos⁡θ\cos\theta implies symmetry about the initial line ("x""x"-axis). We can sketch for 0≤θ≤π0 \le \theta \le \pi and then reflect.

  1. Table of Values: | θ\theta | 00 | π/3\pi/3 | π/2\pi/2 | 2π/32\pi/3 | π\pi | |---|---|---|---|---|---| | cos⁡θ\cos\theta | 11 | 1/21/2 | 00 | −1/2-1/2 | −1-1 | | rr | 66 | 4.54.5 | 33 | 1.51.5 | 00 |
  2. Key Features:
    • Maximum r: Occurs when cos⁡θ=1\cos\theta = 1, so θ=0\theta=0. Max r=3(1+1)=6r = 3(1+1) = 6. The point is (6,0)(6, 0) in Cartesian coordinates.
    • Minimum r: Occurs when cos⁡θ=−1\cos\theta = -1, so θ=π\theta=\pi. Min r=3(1−1)=0r = 3(1-1) = 0. The curve passes through the pole at θ=π\theta=\pi.
    • Tangent at the pole: The tangent at the pole is the line θ=π\theta = \pi (the negative x-axis).
    • When θ=π/2\theta = \pi/2, r=3r=3. The point is (0,3)(0, 3) in Cartesian coordinates.
  3. Sketching:
    • Start at θ=0\theta=0, where the curve is at its furthest point from the pole, (6,0)(6,0).
    • As θ\theta increases to π/2\pi/2, rr decreases from 66 to 33. The curve moves inwards, passing through (0,3)(0,3).
    • As θ\theta increases from π/2\pi/2 to π\pi, rr decreases from 33 to 00, arriving at the pole with a tangent along the line θ=π\theta=\pi.
    • Use symmetry to draw the lower half of the curve for π<θ<2π\pi < \theta < 2\pi. The curve leaves the pole and returns to the starting point (6,0)(6,0). The resulting shape is a cardioid (heart-shape) on its side.

Worked example 2

Find the area of the region enclosed by the curve r=4sin⁡(2θ)r = 4\sin(2\theta) for 0≤θ≤π/20 \le \theta \le \pi/2.

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The curve r=4sin⁡(2θ)r = 4\sin(2\theta) is a four-petalled rose. The given range 0≤θ≤π/20 \le \theta \le \pi/2 corresponds to the first petal in the first quadrant.

  1. Set up the integral: The area AA is given by the formula A=12∫αβr2 dθA = \frac{1}{2} \int_{\alpha}^{\beta} r^2 \, d\theta. Here, r=4sin⁡(2θ)r = 4\sin(2\theta), α=0\alpha=0, and β=π/2\beta=\pi/2. A=12∫0π/2(4sin⁡(2θ))2 dθA = \frac{1}{2} \int_{0}^{\pi/2} (4\sin(2\theta))^2 \, d\theta A=12∫0π/216sin⁡2(2θ) dθA = \frac{1}{2} \int_{0}^{\pi/2} 16\sin^2(2\theta) \, d\theta A=8∫0π/2sin⁡2(2θ) dθA = 8 \int_{0}^{\pi/2} \sin^2(2\theta) \, d\theta
  2. Use a trigonometric identity: We use the double angle identity cos⁡(2A)=1−2sin⁡2(A)\cos(2A) = 1 - 2\sin^2(A), which rearranges to sin⁡2(A)=12(1−cos⁡(2A))\sin^2(A) = \frac{1}{2}(1 - \cos(2A)). Let A=2θA = 2\theta, so sin⁡2(2θ)=12(1−cos⁡(4θ))\sin^2(2\theta) = \frac{1}{2}(1 - \cos(4\theta)). A=8∫0π/212(1−cos⁡(4θ)) dθA = 8 \int_{0}^{\pi/2} \frac{1}{2}(1 - \cos(4\theta)) \, d\theta A=4∫0π/2(1−cos⁡(4θ)) dθA = 4 \int_{0}^{\pi/2} (1 - \cos(4\theta)) \, d\theta
  3. Integrate and evaluate: A=4[θ−14sin⁡(4θ)]0π/2A = 4 \left[ \theta - \frac{1}{4}\sin(4\theta) \right]_{0}^{\pi/2} A=4((π2−14sin⁡(2π))−(0−14sin⁡(0)))A = 4 \left( (\frac{\pi}{2} - \frac{1}{4}\sin(2\pi)) - (0 - \frac{1}{4}\sin(0)) \right) Since sin⁡(2π)=0\sin(2\pi) = 0 and sin⁡(0)=0\sin(0) = 0, this simplifies to: A=4(π2−0−0)A = 4 \left( \frac{\pi}{2} - 0 - 0 \right) A=2πA = 2\pi

The area of one petal is 2π2\pi square units.