Rectangular coordinates locate a point by going across and then up. Polar coordinates locate it by turning to face a direction and then walking a distance. Curves that are messy in x and y, like flowers and heart shapes, often have very simple polar equations. Because x and y can be written in terms of θ, finding slopes is just parametric differentiation with θ as the parameter.
The point (r,θ) is found by turning through angle θ from the positive x-axis (counterclockwise is positive) and moving a distance r from the origin, which is called the pole. Angles are in radians: 2π is a quarter turn and π is a half turn.
If r is negative, you face direction θ and then walk backwards. So (−2,0) is the same point as (2,π). Every point has many polar names: adding 2π to θ gives the same point.
You don’t need to memorize the big fraction: just write x and y in terms of θ and differentiate. Horizontal and vertical tangents work as before: horizontal where dθdy=0 and dθdx=0, vertical where dθdx=0 and dθdy=0.
The distance from the pole is ∣r∣. So dθdr tells you whether the point is moving toward or away from the pole as θ increases:
r>0 and dθdr>0: moving away from the pole.
r>0 and dθdr<0: moving toward the pole.
If r<0, it’s reversed. In short: same signs means away, opposite signs means toward.
Similarly, the sign of dθdy says whether y is increasing (moving up), and the sign of dθdx says whether x is increasing (moving right). AP questions often ask you to interpret these in a sentence.
Start at (2,0) on the positive x-axis. As θ goes to 2π, r shrinks to 1, reaching the point (0,1). At θ=π, r=0: the curve reaches the pole. Then it repeats the same shape below the x-axis and returns to (2,0). The result is the heart-shaped cardioid in the figure, with its point at the pole.
For r=2+3cosθ, is the point on the curve moving toward or away from the pole at (a) θ=2π, (b) θ=43π? Give a reason.
Solution.dθdr=−3sinθ.
(a) At θ=2π: r=2>0 and dθdr=−3<0. Since r>0 and r is decreasing, the distance from the pole is decreasing: the point is moving toward the pole.
(b) At θ=43π: r=2−232≈−0.121<0 and dθdr=−232<0. Now r is negative and getting more negative, so ∣r∣ is increasing: the point is moving away from the pole. (Same signs, so away.) This part of the curve is the limaçon’s inner loop.
Thinking dr/dθ is the slope.dθdr is how fast the distance from the pole changes, not dxdy. For the slope you must go through x=rcosθ and y=rsinθ.
Forgetting the product rule.y=f(θ)sinθ is a product, so dθdy=f′(θ)sinθ+f(θ)cosθ. Dropping either term is a frequent error.
Taking θ straight from the calculator’s inverse tangent.tan−1(xy) only gives angles between −2π and 2π. For points in quadrants II and III, add π.
Ignoring negative r. When r<0, the point is on the opposite side of the pole, and the “toward or away” rule reverses. Check the signs of both r and dθdr.
Degree mode and degree angles. Polar work in AP calculus uses radians throughout. If you learned trig in degrees, convert: 30∘=6π, 45∘=4π, 60∘=3π, 90∘=2π.
1. (Warm-up) Convert (6,6π) to rectangular coordinates.
Solutionx=6cos6π=6⋅23=33,y=6sin6π=6⋅21=3
The point is (33,3).
2. (Warm-up) Convert (−1,3) to polar coordinates with r>0 and 0≤θ<2π.
Solution
r=1+3=2. tanθ=−3 with the point in quadrant II, so θ=32π. The point is (2,32π).
3. (Warm-up) Write r=4cosθ in rectangular form and describe the curve.
Solutionr2=4rcosθ⇒x2+y2=4x⇒(x−2)2+y2=4
A circle with centre (2,0) and radius 2, passing through the pole.
4. (Core) Write each rectangular equation in polar form.
(a) x+y=4
(b) x2+y2=10x
Solution
(a) rcosθ+rsinθ=4, so r=cosθ+sinθ4.
(b) r2=10rcosθ, so r=10cosθ (dividing by r loses nothing, since r=10cosθ already passes through the pole at θ=2π).
5. (Core) For the rose r=4sin(3θ):
(a) How many petals does it have, and how long is each?
(b) The first petal is traced for 0≤θ≤3π. At what angle is its tip?
(c) How many petals does r=4sin(2θ) have?
Solution
(a) n=3 is odd, so 3 petals. The largest value of ∣r∣ is 4, so each petal has length 4.
(b) r=0 at θ=0 and θ=3π, and r is largest when sin(3θ)=1, at 3θ=2π, so θ=6π.
(c) n=2 is even, so 2n=4 petals.
6. (Core) Find the tangent line to the spiral r=θ at θ=2π.
Solution
x=θcosθ and y=θsinθ, so
dθdx=cosθ−θsinθ,dθdy=sinθ+θcosθ
At θ=2π: dθdx=0−2π=−2π and dθdy=1+0=1, so
dxdy=−π/21=−π2
The point is (x,y)=(0,2π). Tangent line: y=−π2x+2π.
7. (Core) Find the points on r=2cosθ, 0≤θ<π, where the tangent line is horizontal.
Solution
x=2cos2θ and y=2sinθcosθ=sin(2θ), so
dθdx=−4cosθsinθ=−2sin(2θ),dθdy=2cos(2θ)
dθdy=0 when 2θ=2π or 23π, so θ=4π or 43π. There dθdx=−2 and 2, both nonzero.
θ=4π: (x,y)=(1,1).
θ=43π: (x,y)=(1,−1).
These are the top and bottom of the circle with centre (1,0) and radius 1, as expected.
8. (Challenge) For the limaçon r=1+2sinθ, decide whether the point on the curve is moving toward or away from the pole at (a) θ=65π and (b) θ=34π. Justify each answer.
Solution
dθdr=2cosθ.
(a) r=1+2⋅21=2>0 and dθdr=2(−23)=−3<0. Opposite signs: ∣r∣ is decreasing, so the point is moving toward the pole.
(b) r=1+2(−23)=1−3≈−0.732<0 and dθdr=2(−21)=−1<0. Same signs: ∣r∣ is increasing, so the point is moving away from the pole.
9. (Challenge) Find all points on the cardioid r=1+cosθ, 0≤θ<2π, where the tangent line is vertical.
dθdx=0 when sinθ=0 (θ=0,π) or cosθ=−21 (θ=32π,34π). Check dθdy at each:
θ=0: 1+1=2=0. Vertical tangent at r=2: the point (2,0).
θ=32π: −21−21=−1=0. Here r=21, so the point is (21cos32π,21sin32π)=(−41,43).
θ=34π: also −1=0. The point is (−41,−43).
θ=π: −1+1=0. Both derivatives are 0 (this is the pole), so this needs more work. Using L’Hôpital’s rule, θ→πlimdx/dθdy/dθ=0, so the tangent at the cusp is horizontal, not vertical.
Vertical tangents: (2,0), (−41,43) and (−41,−43).