Polar Coordinates and Differentiation - AP Calculus BC

  1. Let CC be the polar curve r=3sin⁡(2θ)r = 3\sin(2\theta). What is the rate of change of the radius rr with respect to the angle θ\theta when θ=π4\theta = \frac{\pi}{4}?
    Answer: 00 The rate of change of the radius rr with respect to the angle θ\theta is drdθ\frac{dr}{d\theta}. For r=3sin⁡(2θ)r = 3\sin(2\theta), the derivative is drdθ=3cos⁡(2θ)⋅2=6cos⁡(2θ)\frac{dr}{d\theta} = 3\cos(2\theta) \cdot 2 = 6\cos(2\theta). Evaluating at θ=π4\theta = \frac{\pi}{4} gives drdθ=6cos⁡(2⋅π4)=6cos⁡(π2)=6(0)=0\frac{dr}{d\theta} = 6\cos(2 \cdot \frac{\pi}{4}) = 6\cos(\frac{\pi}{2}) = 6(0) = 0.
  2. A curve is described by r=2sin⁡θr=2\sin\theta; what is dydx\dfrac{dy}{dx} at θ=π2\theta=\dfrac{\pi}{2}?
    Answer: 00 This problem requires the skill of differentiation in polar coordinates to find the slope of the tangent line in Cartesian coordinates. To find dy/dx for a polar curve r = f(θ), use the formula dy/dx = [f'(θ) sin θ + f(θ) cos θ] / [f'(θ) cos θ - f(θ) sin θ]. For r = 2 sin θ, f'(θ) = 2 cos θ, so at θ = π/2, f'(π/2) = 0 and f(π/2) = 2. Plugging in, the numerator is 0·1 + 2·0 = 0 and the denominator is 0·0 - 2·1 = -2, yielding dy/dx = 0/(-2) = 0. A tempting distractor is choice B, dr/dθ at π/2 which is 0, but this fails because while it matches numerically here, it generally ignores the transformation and would not work for other points. When computing polar derivatives, always remember to use the complete formula to account for the coordinate transformation, a strategy applicable to any polar curve.
  3. Which of the following is the slope of a tangent line to the graph of the polar curve r=1−2cos⁡θr = 1 - 2\cos\theta at the pole?
    Answer: 3\sqrt{3} The curve passes through the pole when r=0r=0. So, 1−2cos⁡θ=01 - 2\cos\theta = 0, which gives cos⁡θ=12\cos\theta = \frac{1}{2}. This occurs at θ=π3\theta = \frac{\pi}{3} and θ=5π3\theta = \frac{5\pi}{3}. The slope of the tangent line at the pole is given by tan⁡θ\tan\theta, provided drdθ≠0\frac{dr}{d\theta} \neq 0. Here, drdθ=2sin⁡θ\frac{dr}{d\theta} = 2\sin\theta. At θ=π3\theta = \frac{\pi}{3}, drdθ=2sin⁡(π3)=3≠0\frac{dr}{d\theta} = 2\sin(\frac{\pi}{3}) = \sqrt{3} \neq 0. The slope is tan⁡(π3)=3\tan(\frac{\pi}{3}) = \sqrt{3}. At θ=5π3\theta = \frac{5\pi}{3}, the slope is tan⁡(5π3)=−3\tan(\frac{5\pi}{3}) = -\sqrt{3}. One of these values is 3\sqrt{3}.
  4. For the polar curve r=3−cos⁡θr=3-\cos\theta, what is dydx\dfrac{dy}{dx} at θ=0\theta=0?
    Answer: undefined This problem involves finding dy/dx for r = 3 - cos θ using polar differentiation. The formula is dy/dx = (dr/dθ·sin θ + r·cos θ)/(dr/dθ·cos θ - r·sin θ). With dr/dθ = sin θ, at θ = 0: r = 3 - 1 = 2, dr/dθ = 0, sin(0) = 0, cos(0) = 1. Substituting: dy/dx = (0·0 + 2·1)/(0·1 - 2·0) = 2/0, which is undefined. A common error is assuming dy/dx = 0 when the numerator is finite but the denominator is zero. When the denominator equals zero, dy/dx is undefined, indicating a vertical tangent line at that point.
  5. For the polar curve r=sec⁡θr=\sec\theta, determine dydx\dfrac{dy}{dx} at θ=0\theta=0.
    Answer: undefined This problem requires the skill of differentiation in polar coordinates to find the slope of the tangent line in Cartesian coordinates. To find dy/dxdy/dx for a polar curve r=f(θ)r = f(\theta), use the formula dydx=f′(θ)sin⁡θ+f(θ)cos⁡θf′(θ)cos⁡θ−f(θ)sin⁡θ\dfrac{dy}{dx} = \dfrac{f'(\theta) \sin \theta + f(\theta) \cos \theta}{f'(\theta) \cos \theta - f(\theta) \sin \theta}. For r=sec⁡θr = \sec \theta, f′(θ)=sec⁡θtan⁡θf'(\theta) = \sec \theta \tan \theta, so at θ=0\theta = 0, f′(0)=0f'(0) = 0 and f(0)=1f(0) = 1. Plugging in, the numerator is 0⋅0+1⋅1=10 \cdot 0 + 1 \cdot 1 = 1 and the denominator is 0⋅1−1⋅0=00 \cdot 1 - 1 \cdot 0 = 0, yielding dy/dxdy/dx undefined. A tempting distractor is choice C, drdθ\dfrac{dr}{d\theta} at 0 which is 0, but this fails because it does not reveal the division by zero in the denominator, which indicates a vertical tangent. When computing polar derivatives, always remember to use the complete formula to account for the coordinate transformation, a strategy applicable to any polar curve.
  6. At θ=0\theta=0, the polar curve r=3cos⁡(2θ)r=3\cos(2\theta) has a tangent line that is
    Answer: vertical. For r=3cos⁡(2θ)r=3\cos(2\theta), we have drdθ=−6sin⁡(2θ)\frac{dr}{d\theta}=-6\sin(2\theta). We evaluate the derivatives of x and y at θ=0\theta=0. At θ=0\theta=0, r=3cos⁡(0)=3r=3\cos(0)=3 and drdθ=−6sin⁡(0)=0\frac{dr}{d\theta}=-6\sin(0)=0. Then dydθ=drdθsin⁡θ+rcos⁡θ=(0)sin⁡(0)+(3)cos⁡(0)=3\frac{dy}{d\theta} = \frac{dr}{d\theta}\sin\theta+r\cos\theta = (0)\sin(0)+(3)\cos(0)=3. And dxdθ=drdθcos⁡θ−rsin⁡θ=(0)cos⁡(0)−(3)sin⁡(0)=0\frac{dx}{d\theta} = \frac{dr}{d\theta}\cos\theta-r\sin\theta = (0)\cos(0)-(3)\sin(0)=0. Since dxdθ=0\frac{dx}{d\theta}=0 and dydθ≠0\frac{dy}{d\theta}\neq 0, the tangent line is vertical.
  7. For r=θ2r=\theta^2, what is dydx\dfrac{dy}{dx} at θ=1\theta=1?
    Answer: 2sin⁡1+cos⁡12cos⁡1−sin⁡1\dfrac{2\sin 1+\cos 1}{2\cos 1-\sin 1} This problem requires finding dy/dx for the polar curve r = θ² using polar differentiation techniques. For polar curves, dy/dx = (dy/dθ)/(dx/dθ) where x = r cos θ and y = r sin θ. With r = θ² and r' = 2θ, at θ = 1 we have r = 1 and r' = 2. Computing dx/dθ = -r sin θ + r' cos θ = -1 sin 1 + 2 cos 1 = 2 cos 1 - sin 1 and dy/dθ = r cos θ + r' sin θ = 1 cos 1 + 2 sin 1 = cos 1 + 2 sin 1. Therefore dy/dx = (cos 1 + 2 sin 1)/(2 cos 1 - sin 1) = (2 sin 1 + cos 1)/(2 cos 1 - sin 1). Students might compute dr/dθ = 2 or try tan 1, but these miss the parametric nature of polar curves. Always use the full parametric derivative formula for polar curves, not shortcuts.
  8. What is the slope of the line tangent to the graph of the polar curve r=4cos⁡θr = 4\cos\theta at the point where θ=π3\theta = \frac{\pi}{3}?
    Answer: 13\frac{1}{\sqrt{3}} We use the formula for the slope in polar coordinates: dydx=drdθsin⁡θ+rcos⁡θdrdθcos⁡θ−rsin⁡θ\frac{dy}{dx} = \frac{\frac{dr}{d\theta}\sin\theta + r\cos\theta}{\frac{dr}{d\theta}\cos\theta - r\sin\theta}. For r=4cos⁡θr = 4\cos\theta, we have drdθ=−4sin⁡θ\frac{dr}{d\theta} = -4\sin\theta. Substituting these into the formula gives dydx=(−4sin⁡θ)sin⁡θ+(4cos⁡θ)cos⁡θ(−4sin⁡θ)cos⁡θ−(4cos⁡θ)sin⁡θ=4(cos⁡2θ−sin⁡2θ)−8sin⁡θcos⁡θ=4cos⁡(2θ)−4sin⁡(2θ)=−cot⁡(2θ)\frac{dy}{dx} = \frac{(-4\sin\theta)\sin\theta + (4\cos\theta)\cos\theta}{(-4\sin\theta)\cos\theta - (4\cos\theta)\sin\theta} = \frac{4(\cos^2\theta - \sin^2\theta)}{-8\sin\theta\cos\theta} = \frac{4\cos(2\theta)}{-4\sin(2\theta)} = -\cot(2\theta). At θ=π3\theta = \frac{\pi}{3}, the slope is −cot⁡(2π3)=−(−13)=13- \cot(\frac{2\pi}{3}) = -(-\frac{1}{\sqrt{3}}) = \frac{1}{\sqrt{3}}.
  9. What is the slope of the line tangent to the polar curve r=3θr = 3\theta at the point where θ=π2\theta = \frac{\pi}{2}?
    Answer: −2π-\frac{2}{\pi} To find the slope of the tangent line, we compute dydx=dy/dθdx/dθ\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta}. The Cartesian coordinates are x=rcos⁡θ=3θcos⁡θx = r\cos\theta = 3\theta\cos\theta and y=rsin⁡θ=3θsin⁡θy = r\sin\theta = 3\theta\sin\theta. Using the product rule, we find the derivatives with respect to θ\theta: dxdθ=3cos⁡θ−3θsin⁡θ\frac{dx}{d\theta} = 3\cos\theta - 3\theta\sin\theta and dydθ=3sin⁡θ+3θcos⁡θ\frac{dy}{d\theta} = 3\sin\theta + 3\theta\cos\theta. Evaluating at θ=π2\theta = \frac{\pi}{2} gives dxdθ=3(0)−3(π2)(1)=−3π2\frac{dx}{d\theta} = 3(0) - 3(\frac{\pi}{2})(1) = -\frac{3\pi}{2} and dydθ=3(1)+3(π2)(0)=3\frac{dy}{d\theta} = 3(1) + 3(\frac{\pi}{2})(0) = 3. The slope is dydx=3−3π/2=−2π\frac{dy}{dx} = \frac{3}{-3\pi/2} = -\frac{2}{\pi}.
  10. Consider the polar curve r=2sin⁡θr = 2\sin\theta. What is the value of d2ydx2\frac{d^2y}{dx^2} at θ=π2\theta = \frac{\pi}{2}?
    Answer: −1-1 The curve r=2sin⁡θr=2\sin\theta is a circle of radius 1 centered at (0,1). In Cartesian coordinates, x2+(y−1)2=1x^2 + (y-1)^2 = 1. The point at θ=π2\theta=\frac{\pi}{2} is (x,y)=(0,2)(x,y)=(0,2), which is the top of the circle. At this point, the curve has a horizontal tangent, so dydx=0\frac{dy}{dx}=0. Differentiating x2+y2−2y=0x^2 + y^2 - 2y = 0 implicitly gives 2x+2ydydx−2dydx=02x + 2y\frac{dy}{dx} - 2\frac{dy}{dx} = 0. Differentiating again gives 2+2(dydx)2+2yd2ydx2−2d2ydx2=02 + 2(\frac{dy}{dx})^2 + 2y\frac{d^2y}{dx^2} - 2\frac{d^2y}{dx^2} = 0. At (0,2)(0,2), we know dydx=0\frac{dy}{dx}=0. Substituting these values gives 2+2(0)2+2(2)d2ydx2−2d2ydx2=02 + 2(0)^2 + 2(2)\frac{d^2y}{dx^2} - 2\frac{d^2y}{dx^2} = 0, which simplifies to 2+2d2ydx2=02 + 2\frac{d^2y}{dx^2} = 0. Thus, d2ydx2=−1\frac{d^2y}{dx^2} = -1.
  11. For the polar curve r=θr=\theta, what is dydx\dfrac{dy}{dx} at θ=π2\theta=\dfrac{\pi}{2}?
    Answer: −2π-\dfrac{2}{\pi} This problem involves finding dy/dx for the polar spiral r = θ using polar differentiation. For polar curves, we apply dy/dx = (dy/dθ)/(dx/dθ) where x = r cos θ and y = r sin θ. With r = θ and r' = 1, we get dx/dθ = -θ sin θ + cos θ and dy/dθ = θ cos θ + sin θ. At θ = π/2, we have dx/dθ = -(π/2)(1) + 0 = -π/2 and dy/dθ = (π/2)(0) + 1 = 1. Therefore dy/dx = 1/(-π/2) = -2/π. Students often confuse the reciprocal relationship and write π/2 instead of -2/π. Remember that polar differentiation requires careful application of the product rule to both x(θ) and y(θ).
  12. For the polar curve r=2−sin⁡θr=2-\sin\theta, what is dydx\frac{dy}{dx} at θ=π2\theta=\frac{\pi}{2}?
    Answer: 00 This problem asks for dy/dx of r = 2 - sin θ using polar differentiation. We use dy/dx = (dr/dθ·sin θ + r·cos θ)/(dr/dθ·cos θ - r·sin θ). Given r = 2 - sin θ, we find dr/dθ = -cos θ. At θ = π/2: r = 2 - sin(π/2) = 2 - 1 = 1, dr/dθ = -cos(π/2) = 0, and dy/dx = (0·1 + 1·0)/(0·0 - 1·1) = 0/(-1) = 0. A common mistake is computing dr/dθ incorrectly or mixing up signs in the formula. For polar differentiation, carefully evaluate each component and maintain proper signs throughout the calculation.
  13. For which value of θ\theta in the interval [0,2π)[0, 2\pi) does the polar curve r=1−sin⁡θr = 1 - \sin\theta have a horizontal tangent line?
    Answer: 3π2\frac{3\pi}{2} A horizontal tangent occurs when dydθ=0\frac{dy}{d\theta} = 0 and dxdθ≠0\frac{dx}{d\theta} \neq 0. We have r=1−sin⁡θr = 1 - \sin\theta and drdθ=−cos⁡θ\frac{dr}{d\theta} = -\cos\theta. Then dydθ=drdθsin⁡θ+rcos⁡θ=(−cos⁡θ)sin⁡θ+(1−sin⁡θ)cos⁡θ=cos⁡θ(1−2sin⁡θ)=0\frac{dy}{d\theta} = \frac{dr}{d\theta}\sin\theta + r\cos\theta = (-\cos\theta)\sin\theta + (1 - \sin\theta)\cos\theta = \cos\theta(1 - 2\sin\theta) = 0. This implies cos⁡θ=0\cos\theta = 0 (so θ=π2,3π2\theta = \frac{\pi}{2}, \frac{3\pi}{2}) or sin⁡θ=12\sin\theta = \frac{1}{2} (so θ=π6,5π6\theta = \frac{\pi}{6}, \frac{5\pi}{6}). We also need to check dxdθ=drdθcos⁡θ−rsin⁡θ=(−cos⁡θ)cos⁡θ−(1−sin⁡θ)sin⁡θ=2sin⁡2θ−sin⁡θ−1\frac{dx}{d\theta} = \frac{dr}{d\theta}\cos\theta - r\sin\theta = (-\cos\theta)\cos\theta - (1 - \sin\theta)\sin\theta = 2\sin^2\theta - \sin\theta - 1. At θ=3π2\theta = \frac{3\pi}{2}, dxdθ=2(−1)2−(−1)−1=2≠0\frac{dx}{d\theta} = 2(-1)^2 - (-1) - 1 = 2 \neq 0. At θ=π2\theta=\frac{\pi}{2}, dxdθ=0\frac{dx}{d\theta} = 0, so the slope is indeterminate. Choices B and C are values where dxdθ=0\frac{dx}{d\theta}=0, which correspond to vertical tangents. Thus, the only valid option is θ=3π2\theta = \frac{3\pi}{2}.
  14. For a particle with position given by the polar curve r=1+cos⁡θr = 1 + \cos\theta, what is the rate of change of the x-coordinate with respect to θ\theta at θ=π2\theta = \frac{\pi}{2}?
    Answer: −1-1 The x-coordinate is given by x=rcos⁡θx = r\cos\theta. Substituting r=1+cos⁡θr=1+\cos\theta, we get x=(1+cos⁡θ)cos⁡θ=cos⁡θ+cos⁡2θx = (1+\cos\theta)\cos\theta = \cos\theta + \cos^2\theta. The rate of change of the x-coordinate with respect to θ\theta is dxdθ\frac{dx}{d\theta}. We have dxdθ=−sin⁡θ+2cos⁡θ(−sin⁡θ)=−sin⁡θ(1+2cos⁡θ)\frac{dx}{d\theta} = -\sin\theta + 2\cos\theta(-\sin\theta) = -\sin\theta(1+2\cos\theta). Evaluating at θ=π2\theta = \frac{\pi}{2} gives dxdθ=−sin⁡(π2)(1+2cos⁡(π2))=−1(1+2(0))=−1\frac{dx}{d\theta} = -\sin(\frac{\pi}{2})(1+2\cos(\frac{\pi}{2})) = -1(1+2(0)) = -1.
  15. What is the equation of the line tangent to the polar curve r=2r=2 at θ=π6\theta = \frac{\pi}{6}?
    Answer: y=−3x+4y = -\sqrt{3}x + 4 For r=2r=2, we have drdθ=0\frac{dr}{d\theta}=0. The slope is dydx=0⋅sin⁡θ+2cos⁡θ0⋅cos⁡θ−2sin⁡θ=−cot⁡θ\frac{dy}{dx} = \frac{0 \cdot \sin\theta + 2\cos\theta}{0 \cdot \cos\theta - 2\sin\theta} = -\cot\theta. At θ=π6\theta=\frac{\pi}{6}, the slope is m=−cot⁡(π6)=−3m = -\cot(\frac{\pi}{6}) = -\sqrt{3}. The point of tangency in Cartesian coordinates is x=rcos⁡θ=2cos⁡(π6)=2(32)=3x=r\cos\theta = 2\cos(\frac{\pi}{6}) = 2(\frac{\sqrt{3}}{2})=\sqrt{3} and y=rsin⁡θ=2sin⁡(π6)=2(12)=1y=r\sin\theta = 2\sin(\frac{\pi}{6}) = 2(\frac{1}{2})=1. The equation of the tangent line is y−1=−3(x−3)y-1 = -\sqrt{3}(x-\sqrt{3}), which simplifies to y−1=−3x+3y-1 = -\sqrt{3}x+3, or y=−3x+4y = -\sqrt{3}x+4.
  16. A curve is given by r=2−cos⁡θr=2-\cos\theta; determine dydx\dfrac{dy}{dx} at θ=π\theta=\pi.
    Answer: undefined This problem requires the skill of differentiation in polar coordinates to find the slope of the tangent line in Cartesian coordinates. To find dy/dxdy/dx for a polar curve r=f(θ)r = f(\theta), use the formula dydx=f′(θ)sin⁡θ+f(θ)cos⁡θf′(θ)cos⁡θ−f(θ)sin⁡θ\frac{dy}{dx} = \frac{f'(\theta) \sin \theta + f(\theta) \cos \theta}{f'(\theta) \cos \theta - f(\theta) \sin \theta}. For r=2−cos⁡θr = 2 - \cos \theta, f′(θ)=sin⁡θf'(\theta) = \sin \theta, so at θ=π\theta = \pi, f′(π)=0f'(\pi) = 0 and f(π)=3f(\pi) = 3. Plugging in, the numerator is 0⋅0+3⋅(−1)=−30 \cdot 0 + 3 \cdot (-1) = -3 and the denominator is 0⋅(−1)−3⋅0=00 \cdot (-1) - 3 \cdot 0 = 0, yielding dy/dxdy/dx undefined. A tempting distractor is choice B, drdθ\frac{dr}{d\theta} at π\pi which is 0, but this fails because it misses the zero denominator that signifies a vertical tangent. When computing polar derivatives, always remember to use the complete formula to account for the coordinate transformation, a strategy applicable to any polar curve.
  17. A polar curve is defined by the equation r=f(θ)r = f(\theta) where ff is a differentiable function. If the curve has a horizontal tangent at θ=π3\theta = \frac{\pi}{3} and f(π3)=1f(\frac{\pi}{3}) = 1, what is the value of f′(π3)f'(\frac{\pi}{3})?
    Answer: −13-\frac{1}{\sqrt{3}} A horizontal tangent occurs when dydθ=0\frac{dy}{d\theta} = 0. The formula is dydθ=f′(θ)sin⁡θ+f(θ)cos⁡θ\frac{dy}{d\theta} = f'(\theta)\sin\theta + f(\theta)\cos\theta. At θ=π3\theta = \frac{\pi}{3}, we set this to zero: f′(π3)sin⁡(π3)+f(π3)cos⁡(π3)=0f'(\frac{\pi}{3})\sin(\frac{\pi}{3}) + f(\frac{\pi}{3})\cos(\frac{\pi}{3}) = 0. We are given f(π3)=1f(\frac{\pi}{3}) = 1, and we know sin⁡(π3)=32\sin(\frac{\pi}{3}) = \frac{\sqrt{3}}{2} and cos⁡(π3)=12\cos(\frac{\pi}{3}) = \frac{1}{2}. Substituting these values gives f′(π3)(32)+(1)(12)=0f'(\frac{\pi}{3})\left(\frac{\sqrt{3}}{2}\right) + (1)\left(\frac{1}{2}\right) = 0. This simplifies to f′(π3)32=−12f'(\frac{\pi}{3})\frac{\sqrt{3}}{2} = -\frac{1}{2}. Solving for f′(π3)f'(\frac{\pi}{3}) gives f′(π3)=−13f'(\frac{\pi}{3}) = -\frac{1}{\sqrt{3}}.
  18. The equation of a polar curve is given by r=f(θ)r = f(\theta). Which of the following expressions gives dydx\frac{dy}{dx} in terms of θ\theta?
    Answer: f′(θ)sin⁡θ+f(θ)cos⁡θf′(θ)cos⁡θ−f(θ)sin⁡θ\frac{f'(\theta)\sin\theta + f(\theta)\cos\theta}{f'(\theta)\cos\theta - f(\theta)\sin\theta} The Cartesian coordinates are given by x=rcos⁡θ=f(θ)cos⁡θx = r\cos\theta = f(\theta)\cos\theta and y=rsin⁡θ=f(θ)sin⁡θy = r\sin\theta = f(\theta)\sin\theta. Using the product rule to differentiate with respect to θ\theta gives dxdθ=f′(θ)cos⁡θ−f(θ)sin⁡θ\frac{dx}{d\theta} = f'(\theta)\cos\theta - f(\theta)\sin\theta and dydθ=f′(θ)sin⁡θ+f(θ)cos⁡θ\frac{dy}{d\theta} = f'(\theta)\sin\theta + f(\theta)\cos\theta. The slope is dydx=dy/dθdx/dθ\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta}. The correct expression is f′(θ)sin⁡θ+f(θ)cos⁡θf′(θ)cos⁡θ−f(θ)sin⁡θ\frac{f'(\theta)\sin\theta + f(\theta)\cos\theta}{f'(\theta)\cos\theta - f(\theta)\sin\theta}.
  19. For a particle whose position is described by the polar equation r=θ2r = \theta^2, what is the rate of change of the y-coordinate with respect to θ\theta at θ=π\theta = \pi?
    Answer: −π2-\pi^2 The y-coordinate is given by y=rsin⁡θy = r\sin\theta. Substituting r=θ2r=\theta^2, we get y=θ2sin⁡θy = \theta^2\sin\theta. The rate of change of the y-coordinate with respect to θ\theta is dydθ\frac{dy}{d\theta}. Using the product rule, dydθ=2θsin⁡θ+θ2cos⁡θ\frac{dy}{d\theta} = 2\theta\sin\theta + \theta^2\cos\theta. Evaluating at θ=π\theta = \pi gives dydθ=2πsin⁡π+π2cos⁡π=2π(0)+π2(−1)=−π2\frac{dy}{d\theta} = 2\pi\sin\pi + \pi^2\cos\pi = 2\pi(0) + \pi^2(-1) = -\pi^2.
  20. The slope of the tangent line to a polar curve r=f(θ)r=f(\theta) is given by dydx\frac{dy}{dx}. At a point where f(θ)≠0f(\theta) \neq 0 and f′(θ)≠0f'(\theta) \neq 0, under what condition is the tangent line vertical?
    Answer: drdθcos⁡θ−rsin⁡θ=0\frac{dr}{d\theta} \cos\theta - r \sin\theta = 0 A vertical tangent line occurs when the denominator of dydx\frac{dy}{dx} is zero and the numerator is non-zero. The denominator is dxdθ\frac{dx}{d\theta}. Since x=rcos⁡θx = r\cos\theta, we have dxdθ=drdθcos⁡θ−rsin⁡θ\frac{dx}{d\theta} = \frac{dr}{d\theta}\cos\theta - r\sin\theta. Setting this equal to zero gives the condition for a vertical tangent.

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