Integral Calculus 201-SN3-RE (201-NYB) • CEGEP, Montreal

Revision sheet: polar coordinates, 201-SN3-RE (201-NYB)

This sheet does not explain again how to convert between the two coordinate systems: that fits in two lines. It deals with what decides the mark in 201-SN3-RE (formerly 201-NYB), that is, the fact that a polar representation is not unique and what that does to intersections, then the three factors that the area formula loses most often.

It is written for CEGEP students in the Science program (Sciences de la nature). Once the sheet is read, the corrected exercise set on the same chapter puts every reflex to the test.

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The thread of the chapter

In polar coordinates, rr can be NEGATIVE and the angle is read modulo 2π2\pi: one point has infinitely many representations. That is where every lost mark in the chapter comes from, starting with the intersections that the system of equations never gives.

This chapter is part of 201-SN3-RE (201-NYB), Integral Calculus

The essentials

One point, infinitely many names

  • • Conversion: x=rcos⁡θx=r\cos\theta, y=rsin⁡θy=r\sin\theta; conversely r2=x2+y2r^{2}=x^{2}+y^{2} and tan⁡θ=yx\tan\theta=\frac{y}{x}, watching the QUADRANT.
  • • (r,θ)\left(r,\theta\right) and (r,θ+2kπ)\left(r,\theta+2k\pi\right) designate the same point.
  • • So do (−r,θ)\left(-r,\theta\right) and (r,θ+π)\left(r,\theta+\pi\right): a NEGATIVE radius is read in the opposite direction.
  • • The POLE, the origin of the system, is written (0,θ)\left(0,\theta\right) for any θ\theta: it is the most ambiguous point of the plane.
-1.5-1-0.50.511.5-1.5-1-0.50.511.5r < 0r > 0
The rose r=cos⁡2θr=\cos 2\theta has FOUR petals: two are traced by positive values of rr, two by negative values, in the direction opposite to the angle.

This lack of uniqueness is not a curiosity: it is the direct cause of the two most costly pitfalls of the chapter, missed intersections and loops counted twice.

The formulas of the chapter, with their factors

  • • AREA of a sector: A=12∫αβ[r(θ)]2dθ\mathcal{A}=\frac{1}{2}\int_{\alpha}^{\beta}\left[r(\theta)\right]^{2}d\theta. The 12\frac{1}{2} AND the square are both required.
  • • Area BETWEEN two polar curves: 12∫(rout2−rin2)dθ\frac{1}{2}\int\left(r_{\text{out}}^{2}-r_{\text{in}}^{2}\right)d\theta, a difference of squares.
  • • ARC LENGTH: L=∫αβ[r(θ)]2+[r′(θ)]2 dθL=\int_{\alpha}^{\beta}\sqrt{\left[r(\theta)\right]^{2}+\left[r'(\theta)\right]^{2}}\,d\theta.
  • • SLOPE of the tangent line: dydx=r′sin⁡θ+rcos⁡θr′cos⁡θ−rsin⁡θ\frac{dy}{dx}=\frac{r'\sin\theta+r\cos\theta}{r'\cos\theta-r\sin\theta}, obtained by parametrizing by θ\theta.
dθrarea ≈ ½ r² dθ
The area element is a SECTOR with angle dθd\theta and radius rr, of area 12r2 dθ\frac{1}{2}r^{2}\,d\theta: hence the one half and the square.

The 12\frac{1}{2} in the area comes from the area of a circular sector, 12r2Δθ\frac{1}{2}r^{2}\Delta\theta: the slice is a thin triangle, not a rectangle.

The curves to recognize at a glance

  • • r=ar=a: circle centred at the pole. θ=α\theta=\alpha: line through the pole.
  • • r=2acos⁡θr=2a\cos\theta: circle of radius aa centred at (a,0)(a,0); r=2asin⁡θr=2a\sin\theta: circle centred at (0,a)(0,a).
  • • r=a(1±cos⁡θ)r=a\left(1\pm\cos\theta\right) or a(1±sin⁡θ)a\left(1\pm\sin\theta\right): CARDIOID.
  • • r=acos⁡(nθ)r=a\cos(n\theta): rose with nn petals if nn is ODD, with 2n2n petals if nn is EVEN.
  • • r2=a2cos⁡2θr^{2}=a^{2}\cos 2\theta: lemniscate, shaped like a figure eight lying on its side.
r = ar = 2a cos θcardioidrose
Four shapes to recognize without computing: a circle centred at the pole, a circle through the pole, a cardioid, a rose.

The mistakes that cost marks

These are the errors I correct most often in session. Each one costs marks on a paper, even when the reasoning behind it is right.

1. Rejecting a negative radius

the whole plotting question, since half the petals disappear

What not to write

“r=cos⁡2θr=\cos 2\theta becomes negative between π4\frac{\pi}{4} and 3π4\frac{3\pi}{4}, so the curve does not exist there.”

What to write

“r<0r<0 means the point is plotted in the direction OPPOSITE to θ\theta: these values trace two more petals.”

Why: The polar radius is a signed coordinate, not a distance. A four-petal rose drawn with only two petals signals exactly this mistake, and it shows at first glance on the test.

2. Forgetting the pole in an intersection

the whole question, and a wrong area if the splitting depends on it

What not to write

“1+cos⁡θ=1−cos⁡θ1+\cos\theta=1-\cos\theta gives θ=π2\theta=\frac{\pi}{2} and 3π2\frac{3\pi}{2}: two points of intersection.”

What to write

“There are THREE: the two from the system, plus the POLE, reached by the first curve at θ=π\theta=\pi and by the second at θ=0\theta=0.”

-2.5-2-1.5-1-0.50.511.522.5-2-1.5-1-0.50.511.52poler = 1 + cos θr = 1 − cos θ
The two cardioids cross at three visible points, but the system gives only two: the POLE is reached by each one at a different angle, so it escapes the equation.

Why: The system of equations assumes that the two curves pass through the same point FOR THE SAME angle. At the pole this is not necessary, since (0,θ)\left(0,\theta\right) is the same point for every θ\theta. You must therefore always test the pole SEPARATELY, by solving r=0r=0 for each curve.

3. Forgetting the factor one half in the area

the whole question, since the answer is twice too large

What not to write

A=∫αβr2 dθ\mathcal{A}=\int_{\alpha}^{\beta}r^{2}\,d\theta

What to write

A=12∫αβr2 dθ\mathcal{A}=\frac{1}{2}\int_{\alpha}^{\beta}r^{2}\,d\theta

Why: The elementary slice is a circular sector of area 12r2Δθ\frac{1}{2}r^{2}\Delta\theta, not a rectangle. Immediate check on the circle r=ar=a: the formula must give back πa2\pi a^{2}, which only the version with 12\frac{1}{2} does.

4. Forgetting the square in the area

the whole question

What not to write

A=12∫r dθ\mathcal{A}=\frac{1}{2}\int r\,d\theta

What to write

A=12∫r2 dθ\mathcal{A}=\frac{1}{2}\int r^{2}\,d\theta

Why: Without the square, the expression does not even have the dimension of an area: r dθr\,d\theta is an arc length, not a surface. The dimensional check is enough to rule this version out, and it costs nothing.

5. Integrating over a full turn when one loop is enough

the whole question, since the result counts all four petals

What not to write

“Area of one petal of r=cos⁡2θr=\cos 2\theta: 12∫02πcos⁡22θ dθ\frac{1}{2}\int_{0}^{2\pi}\cos^{2}2\theta\,d\theta.”

What to write

“One petal is traced for θ∈[−π4,π4]\theta\in\left[-\frac{\pi}{4},\frac{\pi}{4}\right]: 12∫−π/4π/4cos⁡22θ dθ=π8\frac{1}{2}\int_{-\pi/4}^{\pi/4}\cos^{2}2\theta\,d\theta=\frac{\pi}{8}.”

-1.5-1-0.50.511.5-1.5-1-0.50.511.5θ = π/4θ = −π/4
One petal of r=cos⁡2θr=\cos 2\theta is traced for θ∈[−π4,π4]\theta\in\left[-\frac{\pi}{4},\frac{\pi}{4}\right]: that is where, and only where, you integrate.

Why: The bounds of a polar area are found by looking for where rr vanishes, that is, where the curve comes back to the pole: those angles delimit a loop. Integrating beyond them counts regions already traced again.

6. Getting the number of petals wrong

1 to 2 marks on the graph

What not to write

“r=cos⁡2θr=\cos 2\theta has two petals, since the coefficient is 22.”

What to write

“An EVEN coefficient gives 2n2n petals, an ODD coefficient gives nn: here n=2n=2, so FOUR petals.”

cos 2θ: 4 petalscos 3θ: 3 petals
cos⁡2θ\cos 2\theta (even coefficient) gives four petals, cos⁡3θ\cos 3\theta (odd) gives three: parity decides.

Why: The rule comes from the sign of rr: when nn is odd, the second half of the turn retraces the same petals with r<0r<0; when nn is even, it traces new ones. Counting the zeros of rr over one turn gives the answer without having to memorize the rule.

7. Confusing the slope of the tangent with the derivative of the radius

the whole question

What not to write

“The tangent line has slope r′(θ)r'(\theta).”

What to write

“dydx=r′sin⁡θ+rcos⁡θr′cos⁡θ−rsin⁡θ\frac{dy}{dx}=\frac{r'\sin\theta+r\cos\theta}{r'\cos\theta-r\sin\theta}, obtained by parametrizing x=rcos⁡θx=r\cos\theta and y=rsin⁡θy=r\sin\theta.”

Why: r′(θ)r'(\theta) measures how fast the point moves away from the pole, not the inclination of the curve. The slope is obtained by treating the curve as parametrized by θ\theta, which brings in two terms on top and two at the bottom through the product rule.

8. Losing the quadrant when converting to polar

the whole question, since the point obtained is its mirror image through the pole

What not to write

“x=−1x=-1, y=−1y=-1 gives tan⁡θ=1\tan\theta=1, so θ=π4\theta=\frac{\pi}{4}.”

What to write

“The point is in the THIRD quadrant: θ=5π4\theta=\frac{5\pi}{4}, and r=2r=\sqrt{2}.”

-1.5-1-0.50.511.5-1.5-1-0.50.511.5π/45π/4(−1, −1)
arctan⁡yx=π4\arctan\frac{y}{x}=\frac{\pi}{4} points to (1,1)(1, 1) (red); the point (−1,−1)(-1, -1) is in the third quadrant, at θ=5π4\theta=\frac{5\pi}{4} (green).

Why: The arctangent function only returns angles between −π2-\frac{\pi}{2} and π2\frac{\pi}{2}: it cannot tell the first quadrant from the third, nor the second from the fourth. A rough sketch of the point, before any computation, settles the question.

Which method to choose

How to find ALL the intersections of two polar curves

The system of equations is never enough. Three checks are needed, in this order.

  • If you are looking for intersections “at the same angle” → solve r1(θ)=r2(θ)r_{1}(\theta)=r_{2}(\theta) over a full turn

    Example: 1+cos⁡θ=1−cos⁡θ1+\cos\theta=1-\cos\theta gives θ=π2\theta=\frac{\pi}{2} and 3π2\frac{3\pi}{2}

  • If you are checking whether the POLE is common → solve r1=0r_{1}=0 and r2=0r_{2}=0 SEPARATELY; if both have a solution, the pole is an intersection

    Example: 1+cos⁡θ=01+\cos\theta=0 at π\pi and 1−cos⁡θ=01-\cos\theta=0 at 00: the pole is common

  • If the two curves can meet with opposite radii → also solve r1(θ)=−r2(θ+π)r_{1}(\theta)=-r_{2}(\theta+\pi)

    Example: useful for roses and lemniscates

  • If a doubt remains → SKETCH both curves: the drawing gives the number of points, the algebra gives their coordinates

    Example: three visible points for two solutions of the system signals a forgotten pole

The drawing is not a proof but a counter: it tells you how many points to look for, which is enough to know whether the system missed some.

Which symmetries to use

A symmetry test takes ten seconds and halves the plotting work, or cuts it to a quarter.

  • If replacing θ\theta with −θ-\theta does not change rr → symmetry about the POLAR AXIS, the x-axis

    Example: r=1+cos⁡θr=1+\cos\theta, since cosine is even

  • If replacing θ\theta with π−θ\pi-\theta does not change rr → symmetry about the line θ=π2\theta=\frac{\pi}{2}, the y-axis

    Example: r=1+sin⁡θr=1+\sin\theta

  • If replacing rr with −r-r, or θ\theta with θ+π\theta+\pi, does not change the curve → symmetry about the POLE

    Example: r2=cos⁡2θr^{2}=\cos 2\theta

  • If no test works → plot point by point over one turn, tabulating rr for the standard angles

    Example: every π12\frac{\pi}{12} is enough for an exam curve

A symmetry test that fails does not prove there is no symmetry: these tests are sufficient, not necessary. So you can try all three without worrying.

How the answer is expected to be written

A marker ticks steps. Here they are in order, with the concluding sentence expected word for word.

A polar area, written for the grader

When to use it: Any question asking for the area of a loop, a petal or a region between two polar curves.

  1. 1 Find the BOUNDS by solving r(θ)=0r(\theta)=0, or by finding the angles of intersection.
  2. 2 Justify that these bounds delimit exactly ONE loop, traced only once.
  3. 3 Write the complete formula with the 12\frac{1}{2} and the square.
  4. 4 Rewrite the squared trigonometric term with the double-angle formulas before integrating.
  5. 5 Compute and conclude with the area unit.

Concluding sentence

The area of the cardioid r=1+cos⁡θr=1+\cos\theta is 12∫02π(1+cos⁡θ)2dθ=3π2\frac{1}{2}\int_{0}^{2\pi}\left(1+\cos\theta\right)^{2}d\theta=\frac{3\pi}{2} square units.

The trap: Integrating cos⁡2θ\cos^{2}\theta without reducing the power. The table does not give this antiderivative directly: you must go through cos⁡2θ=1+cos⁡2θ2\cos^{2}\theta=\frac{1+\cos 2\theta}{2}, and this line is expected on the test.

Marking: Usually 1 mark for the justified bounds, 1 mark for the complete formula, 1 mark for the power reduction, 1 mark for the final computation.

Check before you hand in

Five minutes of checking recover more marks than one more problem started in a hurry.

The typical problem, taken apart

The area of a cardioid, from the bounds to the power reduction

Compute the area of the region inside the cardioid r=1+cos⁡θr=1+\cos\theta.

-1-0.50.511.522.5-2-1.5-1-0.50.511.5r = 1 + cos θ
The cardioid r=1+cos⁡θr=1+\cos\theta reaches its maximum 22 at θ=0\theta=0 and comes back to the pole at θ=π\theta=\pi: one full turn traces it exactly once.

Step 1

Bounds: r=1+cos⁡θr=1+\cos\theta vanishes only at θ=π\theta=\pi, and the curve closes up after one full turn. So we integrate from 00 to 2π2\pi.

Why

Justifying that the turn is traced only ONCE is essential: on a rose, the same reasoning would lead to much narrower bounds, and integrating over 2π2\pi would count all four petals instead of one.

Step 2

Symmetry: cos⁡(−θ)=cos⁡θ\cos(-\theta)=\cos\theta, so r(−θ)=r(θ)r(-\theta)=r(\theta): the curve is symmetric about the polar axis. We can integrate from 00 to π\pi and DOUBLE.

Why

The test takes ten seconds and halves the work. It is optional here but essential on curves where the full integral is heavy.

Step 3

A=12∫02π(1+cos⁡θ)2dθ=12∫02π(1+2cos⁡θ+cos⁡2θ)dθ\mathcal{A}=\frac{1}{2}\int_{0}^{2\pi}\left(1+\cos\theta\right)^{2}d\theta=\frac{1}{2}\int_{0}^{2\pi}\left(1+2\cos\theta+\cos^{2}\theta\right)d\theta.

Why

The 12\frac{1}{2} and the square are written before any expansion: it is the only protection against the two most frequent omissions of the chapter.

Step 4

Power reduction: cos⁡2θ=1+cos⁡2θ2\cos^{2}\theta=\frac{1+\cos 2\theta}{2}, so the integrand becomes 32+2cos⁡θ+cos⁡2θ2\frac{3}{2}+2\cos\theta+\frac{\cos 2\theta}{2}.

Why

No table gives the antiderivative of cos⁡2\cos^{2} directly. The double-angle formula is the only way, and it is the line the marking scheme explicitly expects.

Step 5

On [0,2π]\left[0, 2\pi\right], ∫cos⁡θ dθ=0\int\cos\theta\,d\theta=0 and ∫cos⁡2θ dθ=0\int\cos 2\theta\,d\theta=0: only 32×2π=3π\frac{3}{2}\times 2\pi=3\pi remains. So A=12(3π)=3π2\mathcal{A}=\frac{1}{2}(3\pi)=\frac{3\pi}{2}.

Why

Both cosine terms vanish over a full turn, which makes the computation immediate. Noticing it before integrating saves two lines.

Step 6

Check: the cardioid lies inside the disk of radius 22, of area 4π≈12.574\pi\approx 12.57; the answer 3π2≈4.71\frac{3\pi}{2}\approx 4.71 is a little more than a third of it, which matches the drawing ✓.

Why

Bounding by a simple disk catches the missing factor 22: without the 12\frac{1}{2}, you would have found 3π≈9.423\pi\approx 9.42, almost the whole area of the disk, which is visibly wrong.

The conclusion, written out

The area inside the cardioid r=1+cos⁡θr=1+\cos\theta is 3π2≈4.71\frac{3\pi}{2}\approx 4.71 square units, one and a half times the area of the unit disk.

The classic mistake on this problem: Integrating (1+cos⁡θ)2\left(1+\cos\theta\right)^{2} without reducing cos⁡2θ\cos^{2}\theta, or worse, writing (1+cos⁡θ)2=1+cos⁡2θ\left(1+\cos\theta\right)^{2}=1+\cos^{2}\theta. The cross term 2cos⁡θ2\cos\theta does not disappear, even if it ends up integrating to zero over a full turn.

Learn by heart

  • • x=rcos⁡θx=r\cos\theta, y=rsin⁡θy=r\sin\theta; and for the converse, watch the QUADRANT.
  • • rr can be NEGATIVE: the point is plotted in the direction opposite to θ\theta.
  • • The pole is written (0,θ)\left(0,\theta\right) for every θ\theta: it always escapes the intersection system.
  • • Area: 12∫r2 dθ\frac{1}{2}\int r^{2}\,d\theta. The 12\frac{1}{2} and the square, both of them.
  • • Bounds of a loop: the angles where rr vanishes.
  • • Rose r=acos⁡(nθ)r=a\cos(n\theta): nn petals if nn is odd, 2n2n if nn is even.
  • • Length: ∫r2+[r′]2 dθ\int\sqrt{r^{2}+\left[r'\right]^{2}}\,d\theta.
  • • Reduce cos⁡2\cos^{2} and sin⁡2\sin^{2} before integrating: the table does not give their antiderivatives.

Frequently asked questions

Can the polar radius be negative?

Yes. A negative radius means the point is plotted in the direction opposite to the given angle. This is what allows a rose with an even coefficient to have twice as many petals as its coefficient, half of them being traced with negative values of the radius.

Why does the system of equations not give all the intersections?

Because it assumes that the two curves pass through the same point at the same angle. But the pole has infinitely many names, one for each angle, so two curves can pass through it at different angles. To test the pole, you must therefore solve separately for each radius being zero.

Where does the factor one half in the polar area come from?

From the area of a circular sector, which is half the square of the radius times the angle. The elementary slice of a polar region is a very thin sector, not a rectangle. The immediate check is to apply the formula to a circle of constant radius, which must give back pi times the radius squared.

How do you find the bounds of a polar area?

By looking for the angles where the radius vanishes, because that is where the curve comes back to the pole and closes a loop. For an area between two curves, the bounds are the angles of intersection. Integrating beyond them counts regions already traced again and doubles or quadruples the answer.

How many petals does a polar rose have?

If the coefficient of the angle is odd, the rose has exactly that number of petals. If it is even, it has twice as many. The reason is the sign of the radius: with an odd coefficient, the second half of the turn retraces the same petals, while with an even coefficient it traces new ones.

Practise it

Corrected exercises: Polar coordinates, 201-SN3-RE (201-NYB)

A method is proved on a paper, not on a sheet. The set for the same chapter takes each of these traps into a problem, with the solution written out step by step.

  • 15 corrected exercises
  • 150 points
  • 225 minutes
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© Ahmed Squalli Houssaini. Revision sheet published at www.letuteurscientifique.ca/en/fiches/cegep-calc2-polar-coordinates. Free for personal and classroom use; republishing it elsewhere requires written permission (legal notice).

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