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AP Calculus BC Quiz

AP Calculus BC Quiz: Polar Coordinates And Differentiation

Practice Polar Coordinates And Differentiation in AP Calculus BC with focused quiz questions that help you check what you know, review explanations, and build confidence with test-style prompts.

Question 1 / 20

0 of 20 answered

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\thetar=1−2cosθ at the pole?

Select an answer to continue

What this quiz covers

This quiz focuses on Polar Coordinates And Differentiation, giving you a quick way to practice the rules, question types, and explanations that matter most for AP Calculus BC.

How to use this quiz

Try each quiz question before looking at the correct answer. Use the explanations to review missed ideas, then come back to similar questions until the pattern feels familiar.

All questions

Question 1

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\thetar=1−2cosθ at the pole?

  1. 000
  2. 13\frac{1}{\sqrt{3}}3​1​
  3. 3\sqrt{3}3​ (correct answer)
  4. −3-\sqrt{3}−3​

Explanation: The curve passes through the pole when r=0r=0r=0. So, 1−2cos⁡θ=01 - 2\cos\theta = 01−2cosθ=0, which gives cos⁡θ=12\cos\theta = \frac{1}{2}cosθ=21​. This occurs at θ=π3\theta = \frac{\pi}{3}θ=3π​ and θ=5π3\theta = \frac{5\pi}{3}θ=35π​. The slope of the tangent line at the pole is given by tan⁡θ\tan\thetatanθ, provided drdθ≠0\frac{dr}{d\theta} \neq 0dθdr​=0. Here, drdθ=2sin⁡θ\frac{dr}{d\theta} = 2\sin\thetadθdr​=2sinθ. At θ=π3\theta = \frac{\pi}{3}θ=3π​, drdθ=2sin⁡(π3)=3≠0\frac{dr}{d\theta} = 2\sin(\frac{\pi}{3}) = \sqrt{3} \neq 0dθdr​=2sin(3π​)=3​=0. The slope is tan⁡(π3)=3\tan(\frac{\pi}{3}) = \sqrt{3}tan(3π​)=3​. At θ=5π3\theta = \frac{5\pi}{3}θ=35π​, the slope is tan⁡(5π3)=−3\tan(\frac{5\pi}{3}) = -\sqrt{3}tan(35π​)=−3​. One of these values is 3\sqrt{3}3​.

Question 2

The slope of the tangent line to a polar curve r=f(θ)r=f(\theta)r=f(θ) is given by dydx\frac{dy}{dx}dxdy​. At a point where f(θ)≠0f(\theta) \neq 0f(θ)=0 and f′(θ)≠0f'(\theta) \neq 0f′(θ)=0, under what condition is the tangent line vertical?

  1. drdθsin⁡θ+rcos⁡θ=0\frac{dr}{d\theta} \sin\theta + r \cos\theta = 0dθdr​sinθ+rcosθ=0
  2. drdθcos⁡θ−rsin⁡θ=0\frac{dr}{d\theta} \cos\theta - r \sin\theta = 0dθdr​cosθ−rsinθ=0 (correct answer)
  3. drdθ=0\frac{dr}{d\theta} = 0dθdr​=0
  4. drdθcos⁡θ+rsin⁡θ=0\frac{dr}{d\theta} \cos\theta + r \sin\theta = 0dθdr​cosθ+rsinθ=0

Explanation: A vertical tangent line occurs when the denominator of dydx\frac{dy}{dx}dxdy​ is zero and the numerator is non-zero. The denominator is dxdθ\frac{dx}{d\theta}dθdx​. Since x=rcos⁡θx = r\cos\thetax=rcosθ, we have dxdθ=drdθcos⁡θ−rsin⁡θ\frac{dx}{d\theta} = \frac{dr}{d\theta}\cos\theta - r\sin\thetadθdx​=dθdr​cosθ−rsinθ. Setting this equal to zero gives the condition for a vertical tangent.

Question 3

At θ=0\theta=0θ=0, the polar curve r=3cos⁡(2θ)r=3\cos(2\theta)r=3cos(2θ) has a tangent line that is

  1. horizontal.
  2. vertical. (correct answer)
  3. neither horizontal nor vertical.
  4. undefined because the curve is at the pole.

Explanation: For r=3cos⁡(2θ)r=3\cos(2\theta)r=3cos(2θ), we have drdθ=−6sin⁡(2θ)\frac{dr}{d\theta}=-6\sin(2\theta)dθdr​=−6sin(2θ). We evaluate the derivatives of x and y at θ=0\theta=0θ=0. At θ=0\theta=0θ=0, r=3cos⁡(0)=3r=3\cos(0)=3r=3cos(0)=3 and drdθ=−6sin⁡(0)=0\frac{dr}{d\theta}=-6\sin(0)=0dθdr​=−6sin(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)=3dθdy​=dθdr​sinθ+rcosθ=(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)=0dθdx​=dθdr​cosθ−rsinθ=(0)cos(0)−(3)sin(0)=0. Since dxdθ=0\frac{dx}{d\theta}=0dθdx​=0 and dydθ≠0\frac{dy}{d\theta}\neq 0dθdy​=0, the tangent line is vertical.

Question 4

For which value of θ\thetaθ in the interval [0,2π)[0, 2\pi)[0,2π) does the polar curve r=1−sin⁡θr = 1 - \sin\thetar=1−sinθ have a horizontal tangent line?

  1. π2\frac{\pi}{2}2π​
  2. 7π6\frac{7\pi}{6}67π​
  3. 11π6\frac{11\pi}{6}611π​
  4. 3π2\frac{3\pi}{2}23π​ (correct answer)

Explanation: A horizontal tangent occurs when dydθ=0\frac{dy}{d\theta} = 0dθdy​=0 and dxdθ≠0\frac{dx}{d\theta} \neq 0dθdx​=0. We have r=1−sin⁡θr = 1 - \sin\thetar=1−sinθ and drdθ=−cos⁡θ\frac{dr}{d\theta} = -\cos\thetadθdr​=−cosθ. 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) = 0dθdy​=dθdr​sinθ+rcosθ=(−cosθ)sinθ+(1−sinθ)cosθ=cosθ(1−2sinθ)=0. This implies cos⁡θ=0\cos\theta = 0cosθ=0 (so θ=π2,3π2\theta = \frac{\pi}{2}, \frac{3\pi}{2}θ=2π​,23π​) or sin⁡θ=12\sin\theta = \frac{1}{2}sinθ=21​ (so θ=π6,5π6\theta = \frac{\pi}{6}, \frac{5\pi}{6}θ=6π​,65π​). 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 - 1dθdx​=dθdr​cosθ−rsinθ=(−cosθ)cosθ−(1−sinθ)sinθ=2sin2θ−sinθ−1. At θ=3π2\theta = \frac{3\pi}{2}θ=23π​, dxdθ=2(−1)2−(−1)−1=2≠0\frac{dx}{d\theta} = 2(-1)^2 - (-1) - 1 = 2 \neq 0dθdx​=2(−1)2−(−1)−1=2=0. At θ=π2\theta=\frac{\pi}{2}θ=2π​, dxdθ=0\frac{dx}{d\theta} = 0dθdx​=0, so the slope is indeterminate. Choices B and C are values where dxdθ=0\frac{dx}{d\theta}=0dθdx​=0, which correspond to vertical tangents. Thus, the only valid option is θ=3π2\theta = \frac{3\pi}{2}θ=23π​.

Question 5

For a particle with position given by the polar curve r=1+cos⁡θr = 1 + \cos\thetar=1+cosθ, what is the rate of change of the x-coordinate with respect to θ\thetaθ at θ=π2\theta = \frac{\pi}{2}θ=2π​?

  1. −2-2−2
  2. −1-1−1 (correct answer)
  3. 000
  4. 111

Explanation: The x-coordinate is given by x=rcos⁡θx = r\cos\thetax=rcosθ. Substituting r=1+cos⁡θr=1+\cos\thetar=1+cosθ, we get x=(1+cos⁡θ)cos⁡θ=cos⁡θ+cos⁡2θx = (1+\cos\theta)\cos\theta = \cos\theta + \cos^2\thetax=(1+cosθ)cosθ=cosθ+cos2θ. The rate of change of the x-coordinate with respect to θ\thetaθ is dxdθ\frac{dx}{d\theta}dθdx​. 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)dθdx​=−sinθ+2cosθ(−sinθ)=−sinθ(1+2cosθ). Evaluating at θ=π2\theta = \frac{\pi}{2}θ=2π​ 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)) = -1dθdx​=−sin(2π​)(1+2cos(2π​))=−1(1+2(0))=−1.

Question 6

Consider the polar curve r=2sin⁡θr = 2\sin\thetar=2sinθ. What is the value of d2ydx2\frac{d^2y}{dx^2}dx2d2y​ at θ=π2\theta = \frac{\pi}{2}θ=2π​?

  1. −4-4−4
  2. −1-1−1 (correct answer)
  3. 000
  4. 111

Explanation: The curve r=2sin⁡θr=2\sin\thetar=2sinθ is a circle of radius 1 centered at (0,1). In Cartesian coordinates, x2+(y−1)2=1x^2 + (y-1)^2 = 1x2+(y−1)2=1. The point at θ=π2\theta=\frac{\pi}{2}θ=2π​ is (x,y)=(0,2)(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}=0dxdy​=0. Differentiating x2+y2−2y=0x^2 + y^2 - 2y = 0x2+y2−2y=0 implicitly gives 2x+2ydydx−2dydx=02x + 2y\frac{dy}{dx} - 2\frac{dy}{dx} = 02x+2ydxdy​−2dxdy​=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} = 02+2(dxdy​)2+2ydx2d2y​−2dx2d2y​=0. At (0,2)(0,2)(0,2), we know dydx=0\frac{dy}{dx}=0dxdy​=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} = 02+2(0)2+2(2)dx2d2y​−2dx2d2y​=0, which simplifies to 2+2d2ydx2=02 + 2\frac{d^2y}{dx^2} = 02+2dx2d2y​=0. Thus, d2ydx2=−1\frac{d^2y}{dx^2} = -1dx2d2y​=−1.

Question 7

If a path is modeled by r=sin⁡(2θ)r=\sin(2\theta)r=sin(2θ), what is dydx\frac{dy}{dx}dxdy​ at θ=π4\theta=\frac{\pi}{4}θ=4π​?​

  1. 000
  2. −1-1−1 (correct answer)
  3. drdθ∣θ=π/4=0\frac{dr}{d\theta}\big|_{\theta=\pi/4}=0dθdr​​θ=π/4​=0
  4. 111
  5. 12\frac{1}{\sqrt{2}}2​1​

Explanation: This problem involves finding dy/dx for the rose curve r = sin(2θ) using polar differentiation. The formula is dy/dx = (dr/dθ·sin θ + r·cos θ)/(dr/dθ·cos θ - r·sin θ). First, dr/dθ = 2cos(2θ). At θ = π/4, we have r = sin(2·π/4) = sin(π/2) = 1 and dr/dθ = 2cos(π/2) = 0. Substituting with sin(π/4) = cos(π/4) = 1/√2: dy/dx = (0·(1/√2) + 1·(1/√2))/(0·(1/√2) - 1·(1/√2)) = (1/√2)/(-1/√2) = -1. Choice C incorrectly shows dr/dθ = 0, which is true but not the answer requested. For polar curves, dy/dx depends on both r and dr/dθ values at the given angle.

Question 8

For the polar curve r=3−cos⁡θr=3-\cos\thetar=3−cosθ, what is dydx\dfrac{dy}{dx}dxdy​ at θ=0\theta=0θ=0?

  1. 000
  2. −2-2−2
  3. 222
  4. undefined (correct answer)
  5. −12-\dfrac{1}{2}−21​

Explanation: 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.

Question 9

A polar curve is r=1+2cos⁡θr=1+2\cos\thetar=1+2cosθ. What is dydx\frac{dy}{dx}dxdy​ at θ=π2\theta=\frac{\pi}{2}θ=2π​?

  1. −2-2−2
  2. 12\dfrac{1}{2}21​
  3. 222 (correct answer)
  4. 000
  5. −12-\dfrac{1}{2}−21​

Explanation: This problem requires the skill of differentiating in polar coordinates to find the slope dy/dx. To compute dy/dx for a polar curve, use the formula dy/dx = [ (dr/dθ) sin θ + r cos θ ] / [ (dr/dθ) cos θ - r sin θ ], derived from parametric equations x = r cos θ and y = r sin θ. For r = 1 + 2 cos θ, first compute dr/dθ = -2 sin θ. At θ = π/2, r = 1 and dr/dθ = -2, so the numerator is -2 · 1 + 1 · 0 = -2 and the denominator is -2 · 0 - 1 · 1 = -1, yielding dy/dx = 2. A tempting distractor like 0 might come from mistakenly setting the numerator to zero when cos θ = 0, without computing dr/dθ properly. Always verify the signs in the numerator and denominator of the polar dy/dx formula to capture the correct direction of the tangent line.

Question 10

For the polar curve r=2θ+1r=2\theta+1r=2θ+1, what is dydx\dfrac{dy}{dx}dxdy​ at θ=0\theta=0θ=0?

  1. 000
  2. 12\dfrac{1}{2}21​ (correct answer)
  3. 222
  4. undefined
  5. −12-\dfrac{1}{2}−21​

Explanation: This problem requires finding dy/dx for r = 2θ + 1 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 = 2, at θ = 0: r = 0 + 1 = 1, dr/dθ = 2, sin(0) = 0, cos(0) = 1. Substituting: dy/dx = (2·0 + 1·1)/(2·1 - 1·0) = 1/2. A tempting error is to differentiate r = 2θ + 1 as if it were a Cartesian function, yielding 2. Remember that polar differentiation requires the complete conversion formula, accounting for how both r and θ change along the curve.

Question 11

For the polar curve r=csc⁡θr=\csc\thetar=cscθ, what is dydx\dfrac{dy}{dx}dxdy​ at θ=π4\theta=\dfrac{\pi}{4}θ=4π​?

  1. 000 (correct answer)
  2. 111
  3. −1-1−1
  4. 222
  5. −2-2−2

Explanation: This problem requires finding dy/dx for r = csc θ = 1/sin θ using polar differentiation. The polar derivative formula is dy/dx = (dr/dθ·sin θ + r·cos θ)/(dr/dθ·cos θ - r·sin θ). For r = csc θ, dr/dθ = -csc θ cot θ, and at θ = π/4: r = √2, dr/dθ = -√2·1 = -√2, sin(π/4) = cos(π/4) = 1/√2. Substituting: dy/dx = (-√2·(1/√2) + √2·(1/√2))/(-√2·(1/√2) - √2·(1/√2)) = (-1 + 1)/(-1 - 1) = 0/(-2) = 0. Students might incorrectly treat csc θ as a constant rather than differentiating it properly. Always differentiate r(θ) completely and evaluate all trigonometric functions at the specified angle.

Question 12

For the polar curve r=2sin⁡θ+cos⁡θr=2\sin\theta+\cos\thetar=2sinθ+cosθ, what is dydx\frac{dy}{dx}dxdy​ at θ=π2\theta=\frac{\pi}{2}θ=2π​?

  1. 000
  2. −12-\frac{1}{2}−21​
  3. 12\frac{1}{2}21​ (correct answer)
  4. −1-1−1
  5. 222

Explanation: This problem requires finding dy/dx for a polar curve using the skill of polar differentiation. For polar curves, we use the formula dy/dx = (dy/dθ)/(dx/dθ), where x = r cos θ and y = r sin θ. With r = 2sin θ + cos θ, we find dr/dθ = 2cos θ - sin θ, so at θ = π/2, we have r = 2 and dr/dθ = -1. Computing the derivatives: dy/dθ = (dr/dθ)sin θ + r cos θ = (-1)(1) + (2)(0) = -1, and dx/dθ = (dr/dθ)cos θ - r sin θ = (-1)(0) - (2)(1) = -2. The common error is forgetting the product rule when differentiating x and y with respect to θ. Therefore, dy/dx = -1/(-2) = 1/2, confirming that the key strategy is to carefully apply the product rule to both x = r cos θ and y = r sin θ.

Question 13

For the polar curve r=1+sin⁡θr=1+\sin\thetar=1+sinθ, what is dydx\frac{dy}{dx}dxdy​ at θ=0\theta=0θ=0?

  1. 000
  2. 111 (correct answer)
  3. −1-1−1
  4. 12\frac{1}{2}21​
  5. −12-\frac{1}{2}−21​

Explanation: This problem asks for dy/dx of the cardioid r = 1 + sin θ using polar differentiation. We apply the formula dy/dx = (dr/dθ·sin θ + r·cos θ)/(dr/dθ·cos θ - r·sin θ). Given r = 1 + sin θ, we find dr/dθ = cos θ. At θ = 0: r = 1 + sin(0) = 1, dr/dθ = cos(0) = 1, and dy/dx = (1·0 + 1·1)/(1·1 - 1·0) = 1/1 = 1. A common mistake is using just dr/dθ as the slope without the proper conversion. For polar curves, always use the complete dy/dx formula that accounts for both radial and angular changes.

Question 14

For the polar curve r=2−sin⁡θr=2-\sin\thetar=2−sinθ, what is dydx\frac{dy}{dx}dxdy​ at θ=π2\theta=\frac{\pi}{2}θ=2π​?

  1. −12-\frac{1}{2}−21​
  2. 000 (correct answer)
  3. 12\frac{1}{2}21​
  4. −1-1−1
  5. 111

Explanation: 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.

Question 15

For the polar curve r=1−sin⁡θr=1-\sin\thetar=1−sinθ, find dydx\dfrac{dy}{dx}dxdy​ at θ=0\theta=0θ=0.

  1. −1-1−1 (correct answer)
  2. drdθ∣0\dfrac{dr}{d\theta}\Big|_{0}dθdr​​0​
  3. 000
  4. 111
  5. undefined

Explanation: 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/dxdy/dx for a polar curve r=f(θ)r = f(\theta)r=f(θ), 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}dxdy​=f′(θ)cosθ−f(θ)sinθf′(θ)sinθ+f(θ)cosθ​. For r=1−sin⁡θr = 1 - \sin \thetar=1−sinθ, f′(θ)=−cos⁡θf'(\theta) = -\cos \thetaf′(θ)=−cosθ, so at θ=0\theta = 0θ=0, f′(0)=−1f'(0) = -1f′(0)=−1 and f(0)=1f(0) = 1f(0)=1. Plugging in, the numerator is −1⋅0+1⋅1=1-1 \cdot 0 + 1 \cdot 1 = 1−1⋅0+1⋅1=1 and the denominator is −1⋅1−1⋅0=−1-1 \cdot 1 - 1 \cdot 0 = -1−1⋅1−1⋅0=−1, yielding dy/dx=1/(−1)=−1dy/dx = 1/(-1) = -1dy/dx=1/(−1)=−1. A tempting distractor is choice B, dr/dθdr/d\thetadr/dθ at 0 which is −1-1−1, but this fails because it matches only coincidentally and does not apply the full formula for the slope. When computing polar derivatives, always remember to use the complete formula to account for the coordinate transformation, a strategy applicable to any polar curve.

Question 16

Given the polar curve r=11+sin⁡θr=\dfrac{1}{1+\sin\theta}r=1+sinθ1​, find dydx\frac{dy}{dx}dxdy​ at θ=0\theta=0θ=0.

  1. −1-1−1 (correct answer)
  2. 000
  3. 111
  4. −12-\dfrac{1}{2}−21​
  5. 12\dfrac{1}{2}21​

Explanation: This problem requires the skill of differentiating in polar coordinates to find the slope dy/dx. To compute dy/dx for a polar curve, use the formula dy/dx = [ (dr/dθ) sin θ + r cos θ ] / [ (dr/dθ) cos θ - r sin θ ], derived from parametric equations x = r cos θ and y = r sin θ. For r = 1/(1 + sin θ), first compute dr/dθ = -cos θ / (1 + sin θ)². At θ = 0, r = 1 and dr/dθ = -1, so the numerator is -1 · 0 + 1 · 1 = 1 and the denominator is -1 · 1 - 1 · 0 = -1, yielding dy/dx = -1. A tempting distractor like 0 might arise from incorrectly setting terms to zero without full computation. Always verify the signs in the numerator and denominator of the polar dy/dx formula to capture the correct direction of the tangent line.

Question 17

A curve is given by r=2+sin⁡θr=2+\sin\thetar=2+sinθ. What is dydx\dfrac{dy}{dx}dxdy​ at θ=π2\theta=\dfrac{\pi}{2}θ=2π​?

  1. 000 (correct answer)
  2. 13\dfrac{1}{3}31​
  3. 32\dfrac{3}{2}23​
  4. 111
  5. drdθ∣θ=π/2=0\dfrac{dr}{d\theta}\big|_{\theta=\pi/2}=0dθdr​​θ=π/2​=0

Explanation: This problem requires finding dy/dx for a polar curve using polar differentiation formulas. For polar curves, we use dy/dx = (dy/dθ)/(dx/dθ) where x = r cos θ and y = r sin θ. With r = 2 + sin θ, we get dx/dθ = -r sin θ + r' cos θ = -(2 + sin θ) sin θ + cos θ cos θ and dy/dθ = r cos θ + r' sin θ = (2 + sin θ) cos θ + cos θ sin θ. At θ = π/2, we have r = 3, r' = 0, so dx/dθ = -3(1) + 0 = -3 and dy/dθ = 3(0) + 0 = 0. Many students mistakenly compute dr/dθ instead of dy/dx, but these are different quantities. The key strategy is to always use the parametric chain rule formula dy/dx = (dy/dθ)/(dx/dθ) for polar curves.

Question 18

For the polar curve r=θr=\thetar=θ, what is dydx\dfrac{dy}{dx}dxdy​ at θ=π2\theta=\dfrac{\pi}{2}θ=2π​?

  1. −2π-\dfrac{2}{\pi}−π2​ (correct answer)
  2. π2\dfrac{\pi}{2}2π​
  3. 000
  4. −π2-\dfrac{\pi}{2}−2π​
  5. 2π\dfrac{2}{\pi}π2​

Explanation: 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).

Question 19

What is the slope of the line tangent to the polar curve r=3θr = 3\thetar=3θ at the point where θ=π2\theta = \frac{\pi}{2}θ=2π​?

  1. −π2-\frac{\pi}{2}−2π​
  2. −2π-\frac{2}{\pi}−π2​ (correct answer)
  3. 000
  4. 333

Explanation: To find the slope of the tangent line, we compute dydx=dy/dθdx/dθ\frac{dy}{dx} = \frac{dy/d\theta}{dx/d\theta}dxdy​=dx/dθdy/dθ​. The Cartesian coordinates are x=rcos⁡θ=3θcos⁡θx = r\cos\theta = 3\theta\cos\thetax=rcosθ=3θcosθ and y=rsin⁡θ=3θsin⁡θy = r\sin\theta = 3\theta\sin\thetay=rsinθ=3θsinθ. Using the product rule, we find the derivatives with respect to θ\thetaθ: dxdθ=3cos⁡θ−3θsin⁡θ\frac{dx}{d\theta} = 3\cos\theta - 3\theta\sin\thetadθdx​=3cosθ−3θsinθ and dydθ=3sin⁡θ+3θcos⁡θ\frac{dy}{d\theta} = 3\sin\theta + 3\theta\cos\thetadθdy​=3sinθ+3θcosθ. Evaluating at θ=π2\theta = \frac{\pi}{2}θ=2π​ gives dxdθ=3(0)−3(π2)(1)=−3π2\frac{dx}{d\theta} = 3(0) - 3(\frac{\pi}{2})(1) = -\frac{3\pi}{2}dθdx​=3(0)−3(2π​)(1)=−23π​ and dydθ=3(1)+3(π2)(0)=3\frac{dy}{d\theta} = 3(1) + 3(\frac{\pi}{2})(0) = 3dθdy​=3(1)+3(2π​)(0)=3. The slope is dydx=3−3π/2=−2π\frac{dy}{dx} = \frac{3}{-3\pi/2} = -\frac{2}{\pi}dxdy​=−3π/23​=−π2​.

Question 20

What is the slope of the line tangent to the graph of the polar curve r=4cos⁡θr = 4\cos\thetar=4cosθ at the point where θ=π3\theta = \frac{\pi}{3}θ=3π​?

  1. 3\sqrt{3}3​
  2. 13\frac{1}{\sqrt{3}}3​1​ (correct answer)
  3. −13-\frac{1}{\sqrt{3}}−3​1​
  4. −3-\sqrt{3}−3​

Explanation: 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}dxdy​=dθdr​cosθ−rsinθdθdr​sinθ+rcosθ​. For r=4cos⁡θr = 4\cos\thetar=4cosθ, we have drdθ=−4sin⁡θ\frac{dr}{d\theta} = -4\sin\thetadθdr​=−4sinθ. 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)dxdy​=(−4sinθ)cosθ−(4cosθ)sinθ(−4sinθ)sinθ+(4cosθ)cosθ​=−8sinθcosθ4(cos2θ−sin2θ)​=−4sin(2θ)4cos(2θ)​=−cot(2θ). At θ=π3\theta = \frac{\pi}{3}θ=3π​, the slope is −cot⁡(2π3)=−(−13)=13- \cot(\frac{2\pi}{3}) = -(-\frac{1}{\sqrt{3}}) = \frac{1}{\sqrt{3}}−cot(32π​)=−(−3​1​)=3​1​.