Area and Arc Length in Polar Coordinates

In the rectangular coordinate system, the definite integral provides a way to calculate the area under a curve. In particular, if we have a function y=f(x)

defined from x=a

to x=b

where f(x)>0

on this interval, the area between the curve and the x-axis is given by A=abf(x)dx.

This fact, along with the formula for evaluating this integral, is summarized in the Fundamental Theorem of Calculus. Similarly, the arc length of this curve is given by L=ab1+(f(x))2dx.

In this section, we study analogous formulas for area and arc length in the polar coordinate system.

Areas of Regions Bounded by Polar Curves

We have studied the formulas for area under a curve defined in rectangular coordinates and parametrically defined curves. Now we turn our attention to deriving a formula for the area of a region bounded by a polar curve. Recall that the proof of the Fundamental Theorem of Calculus used the concept of a Riemann sum to approximate the area under a curve by using rectangles. For polar curves we use the Riemann sum again, but the rectangles are replaced by sectors of a circle.

Consider a curve defined by the function r=f(θ),

where αθβ.

Our first step is to partition the interval [α,β]

into n equal-width subintervals. The width of each subinterval is given by the formula Δθ=(βα)/n,

and the ith partition point θi

is given by the formula θi=α+iΔθ.

Each partition point θ=θi

defines a line with slope tanθi

passing through the pole as shown in the following graph.

On the polar coordinate plane, a curve is drawn in the first quadrant, and there are rays from the origin that intersect this curve at a regular interval. Every time one of these rays intersects the curve, a perpendicular line is made from the ray to the next ray. The first instance of a ray-curve intersection is labeled θ = α; the last instance is labeled θ = β. The intervening ones are marked θ1, θ2, …, θn−1.

The line segments are connected by arcs of constant radius. This defines sectors whose areas can be calculated by using a geometric formula. The area of each sector is then used to approximate the area between successive line segments. We then sum the areas of the sectors to approximate the total area. This approach gives a Riemann sum approximation for the total area. The formula for the area of a sector of a circle is illustrated in the following figure.

A circle is drawn with radius r and a sector of angle θ. It is noted that A = (1/2) θ r2.

Recall that the area of a circle is A=πr2.

When measuring angles in radians, 360 degrees is equal to 2π

radians. Therefore a fraction of a circle can be measured by the central angle θ.

The fraction of the circle is given by θ2π,

so the area of the sector is this fraction multiplied by the total area:

A=(θ2π)πr2=12θr2.

Since the radius of a typical sector in [link] is given by ri=f(θi),

the area of the ith sector is given by

Ai=12(Δθ)(f(θi))2.

Therefore a Riemann sum that approximates the area is given by

An=i=1nAii=1n12(Δθ)(f(θi))2.

We take the limit as n

to get the exact area:

A=limnAn=12αβ(f(θ))2dθ.

This gives the following theorem.

Area of a Region Bounded by a Polar Curve

Suppose f

is continuous and nonnegative on the interval αθβ

with 0<βα2π.

The area of the region bounded by the graph of r=f(θ)

between the radial lines θ=α

and θ=β

is

A=12αβ[f(θ)]2dθ=12αβr2dθ.
Finding an Area of a Polar Region

Find the area of one petal of the rose defined by the equation r=3sin(2θ).

The graph of r=3sin(2θ)

follows.

A four-petaled rose with furthest extent 3 from the origin at π/4, 3π/4, 5π/4, and 7π/4.

When θ=0

we have r=3sin(2(0))=0.

The next value for which r=0

is θ=π/2.

This can be seen by solving the equation 3sin(2θ)=0

for θ.

Therefore the values θ=0

to θ=π/2

trace out the first petal of the rose. To find the area inside this petal, use [link] with f(θ)=3sin(2θ),

α=0,

and β=π/2:

A=12αβ[f(θ)]2dθ=120π/2[3sin(2θ)]2dθ=120π/29sin2(2θ)dθ.

To evaluate this integral, use the formula sin2α=(1cos(2α))/2

with α=2θ:

A=120π/29sin2(2θ)dθ=920π/2(1cos(4θ))2dθ=94(0π/21cos(4θ)dθ)=94(θsin(4θ)4)0π/2=94(π2sin2π4)94(0sin4(0)4)=9π8.

Find the area inside the cardioid defined by the equation r=1cosθ.

A=3π/2
Hint

Use [link]. Be sure to determine the correct limits of integration before evaluating.

[link] involved finding the area inside one curve. We can also use [link] to find the area between two polar curves. However, we often need to find the points of intersection of the curves and determine which function defines the outer curve or the inner curve between these two points.

Finding the Area between Two Polar Curves

Find the area outside the cardioid r=2+2sinθ

and inside the circle r=6sinθ.

First draw a graph containing both curves as shown.

A cardioid with equation r = 2 + 2 sinθ is shown, so it has its upper heart part at the origin and the rest of the cardioid is pointed up. There is a circle with radius 6 centered at (3, π/2). The area above the cardioid but below the circle is shaded orange.

To determine the limits of integration, first find the points of intersection by setting the two functions equal to each other and solving for θ:

6sinθ=2+2sinθ4sinθ=2sinθ=12.

This gives the solutions θ=π6

and θ=5π6,

which are the limits of integration. The circle r=3sinθ

is the red graph, which is the outer function, and the cardioid r=2+2sinθ

is the blue graph, which is the inner function. To calculate the area between the curves, start with the area inside the circle between θ=π6

and θ=5π6,

then subtract the area inside the cardioid between θ=π6

and θ=5π6:

A=circlecardioid=12π/65π/6[6sinθ]2dθ12π/65π/6[2+2sinθ]2dθ=12π/65π/636sin2θdθ12π/65π/64+8sinθ+4sin2θdθ=18π/65π/61cos(2θ)2dθ2π/65π/61+2sinθ+1cos(2θ)2dθ=9[θsin(2θ)2]π/65π/62[3θ22cosθsin(2θ)4]π/65π/6=9(5π6sin2(5π/6)2)9(π6sin2(π/6)2)(3(5π6)4cos5π6sin2(5π/6)2)+(3(π6)4cosπ6sin2(π/6)2)=4π.

Find the area inside the circle r=4cosθ

and outside the circle r=2.

A=4π3+43
Hint

Use [link] and take advantage of symmetry.

In [link] we found the area inside the circle and outside the cardioid by first finding their intersection points. Notice that solving the equation directly for θ

yielded two solutions: θ=π6

and θ=5π6.

However, in the graph there are three intersection points. The third intersection point is the origin. The reason why this point did not show up as a solution is because the origin is on both graphs but for different values of θ.

For example, for the cardioid we get

2+2sinθ=0sinθ=−1,

so the values for θ

that solve this equation are θ=3π2+2nπ,

where n is any integer. For the circle we get

6sinθ=0.

The solutions to this equation are of the form θ=nπ

for any integer value of n. These two solution sets have no points in common. Regardless of this fact, the curves intersect at the origin. This case must always be taken into consideration.

Arc Length in Polar Curves

Here we derive a formula for the arc length of a curve defined in polar coordinates.

In rectangular coordinates, the arc length of a parameterized curve (x(t),y(t))

for atb

is given by

L=ab(dxdt)2+(dydt)2dt.

In polar coordinates we define the curve by the equation r=f(θ),

where αθβ.

In order to adapt the arc length formula for a polar curve, we use the equations

x=rcosθ=f(θ)cosθandy=rsinθ=f(θ)sinθ,

and we replace the parameter t by θ.

Then

dxdθ=f(θ)cosθf(θ)sinθdydθ=f(θ)sinθ+f(θ)cosθ.

We replace dt

by dθ,

and the lower and upper limits of integration are α

and β,

respectively. Then the arc length formula becomes

L=ab(dxdt)2+(dydt)2dt=αβ(dxdθ)2+(dydθ)2dθ=αβ(f(θ)cosθf(θ)sinθ)2+(f(θ)sinθ+f(θ)cosθ)2dθ=αβ(f(θ))2(cos2θ+sin2θ)+(f(θ))2(cos2θ+sin2θ)dθ=αβ(f(θ))2+(f(θ))2dθ=αβr2+(drdθ)2dθ.

This gives us the following theorem.

Arc Length of a Curve Defined by a Polar Function

Let f

be a function whose derivative is continuous on an interval αθβ.

The length of the graph of r=f(θ)

from θ=α

to θ=β

is

L=αβ[f(θ)]2+[f(θ)]2dθ=αβr2+(drdθ)2dθ.
Finding the Arc Length of a Polar Curve

Find the arc length of the cardioid r=2+2cosθ.

When θ=0,r=2+2cos0=4.

Furthermore, as θ

goes from 0

to 2π,

the cardioid is traced out exactly once. Therefore these are the limits of integration. Using f(θ)=2+2cosθ,

α=0,

and β=2π,

[link] becomes

L=αβ[ f(θ) ]2+[ f(θ) ]2dθ=02π[ 2+2cosθ ]2+[ 2sinθ ]2dθ=02π4+8cosθ+4cos2θ+4sin2θdθ=02π4+8cosθ+4(cos2θ+sin2θ)dθ=02π8+8cosθdθ=202π2+2cosθdθ.

Next, using the identity cos(2α)=2cos2α1,

add 1 to both sides and multiply by 2. This gives 2+2cos(2α)=4cos2α.

Substituting α=θ/2

gives 2+2cosθ=4cos2(θ/2),

so the integral becomes

L=202π2+2cosθdθ=202π4cos2(θ2)dθ=202π2\|cos(θ2)\|dθ.

The absolute value is necessary because the cosine is negative for some values in its domain. To resolve this issue, change the limits from 0

to π

and double the answer. This strategy works because cosine is positive between 0

and π2.

Thus,

L=402π\|cos(θ2)\|dθ=80πcos(θ2)dθ=8(2sin(θ2))0π=16.

Find the total arc length of r=3sinθ.

s=3π
Hint

Use [link]. To determine the correct limits, make a table of values.

Key Concepts

Key Equations

For the following exercises, determine a definite integral that represents the area.

Region enclosed by r=4

Region enclosed by r=3sinθ

920πsin2θdθ

Region in the first quadrant within the cardioid r=1+sinθ

Region enclosed by one petal of r=8sin(2θ)

320π/2sin2(2θ)dθ

Region enclosed by one petal of r=cos(3θ)

Region below the polar axis and enclosed by r=1sinθ

12π2π(1sinθ)2dθ

Region in the first quadrant enclosed by r=2cosθ

Region enclosed by the inner loop of r=23sinθ

sin−1(2/3)π/2(23sinθ)2dθ

Region enclosed by the inner loop of r=34cosθ

Region enclosed by r=12cosθ

and outside the inner loop

0π(12cosθ)2dθ0π/3(12cosθ)2dθ

Region common to r=3sinθandr=2sinθ

Region common to r=2andr=4cosθ

40π/3dθ+16π/3π/2(cos2θ)dθ

Region common to r=3cosθandr=3sinθ

For the following exercises, find the area of the described region.

Enclosed by r=6sinθ

9π

Above the polar axis enclosed by r=2+sinθ

Below the polar axis and enclosed by r=2cosθ

9π4

Enclosed by one petal of r=4cos(3θ)

Enclosed by one petal of r=3cos(2θ)

9π8

Enclosed by r=1+sinθ

Enclosed by the inner loop of r=3+6cosθ

18π2732

Enclosed by r=2+4cosθ

and outside the inner loop

Common interior of r=4sin(2θ)andr=2

43(4π33)

Common interior of r=32sinθandr=−3+2sinθ

Common interior of r=6sinθandr=3

32(4π33)

Inside r=1+cosθ

and outside r=cosθ

Common interior of r=2+2cosθandr=2sinθ

2π4

For the following exercises, find a definite integral that represents the arc length.

r=4cosθon the interval0θπ2
r=1+sinθ

on the interval 0θ2π

02π(1+sinθ)2+cos2θdθ
r=2secθon the interval0θπ3
r=eθon the interval0θ1
201eθdθ

For the following exercises, find the length of the curve over the given interval.

r=6on the interval0θπ2
r=e3θon the interval0θ2
103(e61)
r=6cosθon the interval0θπ2
r=8+8cosθon the interval0θπ

32

r=1sinθon the interval0θ2π

For the following exercises, use the integration capabilities of a calculator to approximate the length of the curve.

[T] r=3θon the interval0θπ2

6.238

[T] r=2θon the intervalπθ2π

[T] r=sin2(θ2)on the interval0θπ

2

[T] r=2θ2on the interval0θπ

[T] r=sin(3cosθ)on the interval0θπ

4.39

For the following exercises, use the familiar formula from geometry to find the area of the region described and then confirm by using the definite integral.

r=3sinθon the interval0θπ
r=sinθ+cosθon the interval0θπ
A=π(22)2=π2and120π(1+2sinθcosθ)dθ=π2
r=6sinθ+8cosθon the interval0θπ

For the following exercises, use the familiar formula from geometry to find the length of the curve and then confirm using the definite integral.

r=3sinθon the interval0θπ
C=2π(32)=3πand0π3dθ=3π
r=sinθ+cosθon the interval0θπ
r=6sinθ+8cosθon the interval0θπ
C=2π(5)=10πand0π10dθ=10π

Verify that if y=rsinθ=f(θ)sinθ

then dydθ=f(θ)sinθ+f(θ)cosθ.

For the following exercises, find the slope of a tangent line to a polar curve r=f(θ).

Let x=rcosθ=f(θ)cosθ

and y=rsinθ=f(θ)sinθ,

so the polar equation r=f(θ)

is now written in parametric form.

Use the definition of the derivative dydx=dy/dθdx/dθ

and the product rule to derive the derivative of a polar equation.

dydx=f(θ)sinθ+f(θ)cosθf(θ)cosθf(θ)sinθ
r=1sinθ; (12,π6)
r=4cosθ; (2,π3)

The slope is 13.

r=8sinθ; (4,5π6)
r=4+sinθ; (3,3π2)

The slope is 0.

r=6+3cosθ; (3,π)
r=4cos(2θ);

tips of the leaves

At (4,0),

the slope is undefined. At (−4,π2),

the slope is 0.

r=2sin(3θ);

tips of the leaves

r=2θ; (π2,π4)

The slope is undefined at θ=π4.

Find the points on the interval πθπ

at which the cardioid r=1cosθ

has a vertical or horizontal tangent line.

For the cardioid r=1+sinθ,

find the slope of the tangent line when θ=π3.

Slope = −1.

For the following exercises, find the slope of the tangent line to the given polar curve at the point given by the value of θ.

r=3cosθ,θ=π3
r=θ, θ=π2

Slope is −2π.

r=lnθ, θ=e

[T] Use technology: r=2+4cosθ

at θ=π6

Calculator answer: −0.836.

For the following exercises, find the points at which the following polar curves have a horizontal or vertical tangent line.

r=4cosθ
r2=4cos(2θ)

Horizontal tangent at (±2,π6),

(±2,π6).
r=2sin(2θ)

The cardioid r=1+sinθ

Horizontal tangents at π2,7π6,11π6.

Vertical tangents at π6,5π6

and also at the pole (0,0).

Show that the curve r=sinθtanθ

(called a cissoid of Diocles) has the line x=1

as a vertical asymptote.


Creative Commons License
This work is licensed under a Creative Commons Attribution 4.0 International License.

You can also download for free at http://cnx.org/contents/9a1df55a-b167-4736-b5ad-15d996704270@5.1

Attribution: