Skills

Polar Coordinates and Polar Graphs

every AB topic, then series

4 min readfreeNot practiced

Rectangular coordinates say "go xx units right and yy units up". Polar coordinates say "turn to an angle, then go a distance". The 2025 exam's polar question had the lowest average of any question that year, and the readers' advice was simple: review the precalculus first. This page is that review.

Naming a point with (r,θ)(r, \theta)

Start at the pole (the origin). The angle θ\theta is measured from the positive xx-axis, counterclockwise, in radians. Turn to the ray at angle θ\theta, then go rr units along it. That point is (r,θ)(r, \theta).

A polar grid with circles of radius 1 to 4 and rays every π/6. Point P has r = 3 and θ = π/3: its legs are x = r cos θ = 1.5 and y = r sin θ = 3√3/2, about 2.598. Point Q has r = −2 and θ = π/4: it lies 2 units from the pole on the ray opposite θ = π/4, at x = −√2, y = −√2. A side panel lists x = r cos θ, y = r sin θ and r² = x² + y².
Figure 1. P=(3,π3)P = (3, \frac{\pi}{3}) and Q=(−2,π4)Q = (-2, \frac{\pi}{4}), with the legs that give xx and yy. LevlPrep original diagram.

Two facts make polar different from rectangular:

  • rr can be negative. Then you go |r||r| units backward, through the pole, onto the opposite ray. The figure shows Q=(−2,π4)Q = (-2, \frac{\pi}{4}), which sits in the third quadrant.
  • A point has many names. (2,π4)(2, \frac{\pi}{4}), (2,9π4)(2, \frac{9\pi}{4}) and (−2,5π4)(-2, \frac{5\pi}{4}) are the same point. Adding 2π2\pi to θ\theta changes nothing; adding π\pi and flipping the sign of rr changes nothing.

Converting between polar and rectangular

The segment from the pole to (r,θ)(r, \theta) is the hypotenuse of a right triangle with legs xx and yy:

x=rcos⁡θ,y=rsin⁡θ,r2=x2+y2,tan⁡θ=yx.x = r\cos\theta, \qquad y = r\sin\theta, \qquad r^2 = x^2 + y^2, \qquad \tan\theta = \frac{y}{x}.

Worked example 1. Convert (4,5π6)(4, \frac{5\pi}{6}) to rectangular, then convert (0,−5)(0, -5) to polar.

xx=4cos⁡5π6= 4\cos\frac{5\pi}{6}=4⋅(−32)= 4 \cdot \left(-\frac{\sqrt{3}}{2}\right)=−23= -2\sqrt{3} and yy=4sin⁡5π6= 4\sin\frac{5\pi}{6}=4⋅12= 4 \cdot \frac{1}{2}=2= 2. The point is (−23,2)(-2\sqrt{3}, 2).

For (0,−5)(0, -5): r=0+25=5r = \sqrt{0 + 25} = 5. The point is straight down, on the ray θ=3π2\theta = \frac{3\pi}{2}. So (5,3π2)(5, \frac{3\pi}{2}), or equally (−5,π2)(-5, \frac{\pi}{2}).

Do not trust tan⁡θ=yx\tan\theta = \frac{y}{x} alone: (1,−1)(1, -1) and (−1,1)(-1, 1) have the same tangent. Always check the quadrant.

The same formulas convert equations. To rewrite r=6cos⁡θr = 6\cos\theta, multiply by rr: r2=6rcos⁡θr^2 = 6r\cos\theta, so x2+y2=6xx^2 + y^2 = 6x, which is (x−3)2+y2=9(x - 3)^2 + y^2 = 9: a circle of radius 3 through the pole.

Plotting a polar curve from a table

A polar curve r=f(θ)r = f(\theta) gives one distance for each angle. To sketch one, make a table, then sweep around like a lighthouse beam, marking each distance on its ray.

Worked example 2. Sketch r=1+2cos⁡θr = 1 + 2\cos\theta for 0≤θ≤2π0 \le \theta \le 2\pi.

θ\theta00π3\frac{\pi}{3}π2\frac{\pi}{2}2π3\frac{2\pi}{3}π\pi4π3\frac{4\pi}{3}3π2\frac{3\pi}{2}2π2\pi
rr33221100−1-1001133

From θ=0\theta = 0 to 2π3\frac{2\pi}{3} the distance shrinks from 3 to 0: a big arc into the pole. From 2π3\frac{2\pi}{3} to 4π3\frac{4\pi}{3}, rr is negative, so the rays point left but the points land on the right: a small inner loop. From 4π3\frac{4\pi}{3} to 2π2\pi, rr grows back to 3 below the axis.

Two readings matter most for calculus: where r=0r = 0 (the curve passes through the pole) and where rr changes sign (the curve switches to the opposite ray).

Shapes to recognize

Three polar graphs drawn from their equations. Left: the cardioid r = 2 + 2 cos θ, a heart shape reaching 4 units right of the pole and touching the pole once, at θ = π. Middle: the limaçon r = 1 + 2 cos θ, a large loop with a small inner loop, in vermillion, traced while r is negative for 2π/3 < θ < 4π/3. Right: the rose r = 3 sin(2θ), four petals of length 3, one for every π/2 of θ.
Figure 2. A cardioid, a limaçon with an inner loop, and a four-petal rose. LevlPrep original diagram.
EquationShapeWhat to read off
r=ar = acircle centered at the poleradius |a||a|
θ=c\theta = cline through the poleslope tan⁡c\tan c
r=acos⁡θr = a\cos\theta, r=asin⁡θr = a\sin\thetacircle through the polediameter |a||a|, on the xx-axis or yy-axis
r=a+acos⁡θr = a + a\cos\thetacardioidtouches the pole once
r=a+bcos⁡θr = a + b\cos\theta, |a|<|b||a| < |b|limaçon with an inner looploop where r<0r < 0
r=asin⁡(nθ)r = a\sin(n\theta), r=acos⁡(nθ)r = a\cos(n\theta)rosenn petals if nn is odd, 2n2n if nn is even; length |a||a|

A rose r=3sin⁡(2θ)r = 3\sin(2\theta) has four petals (the figure): one for each stretch of θ\theta of length π2\frac{\pi}{2} between zeros of rr. On a graphing calculator, use polar mode and radians, and set the θ\theta-window to 0≤θ≤2π0 \le \theta \le 2\pi to see the whole curve.

Why calculus cares

Writing x=f(θ)cos⁡θx = f(\theta)\cos\theta and y=f(θ)sin⁡θy = f(\theta)\sin\theta turns a polar curve into a parametric curve with parameter θ\theta. Everything from Topics 9.1 to 9.3 then applies: slopes in 9.7, and areas built from thin sectors in 9.8 and 9.9.

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