PARAMETRIC EQUATIONS AND POLAR COORDINATESrfrith.uaa.alaska.edu/M201/Chapter10/Chap10_Sec4.pdf ·...

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PARAMETRIC EQUATIONS AND POLAR COORDINATES 10

Transcript of PARAMETRIC EQUATIONS AND POLAR COORDINATESrfrith.uaa.alaska.edu/M201/Chapter10/Chap10_Sec4.pdf ·...

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PARAMETRIC EQUATIONS AND POLAR COORDINATES

10

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10.4Areas and Lengths

in Polar Coordinates

In this section, we will:

Develop the formula for the area of a region

whose boundary is given by a polar equation.

PARAMETRIC EQUATIONS & POLAR COORDINATES

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AREAS IN POLAR COORDINATES

We need to use the formula for the area of a sector of a circle

A = ½r2θwhere:

r is the radius. θ is the radian measure

of the central angle.

Formula 1

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AREAS IN POLAR COORDINATES

Formula 1 follows from the fact that the area of a sector is proportional to its central angle:

A = (θ/2π)πr2 = ½r2θ

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AREAS IN POLAR COORDINATES

Let R be the region bounded by the polar curve r = f(θ) and by the rays θ = a and θ = b, where:

f is a positive continuous function.

0 < b – a ≤ 2π

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AREAS IN POLAR COORDINATES

We divide the interval [a, b] into subintervalswith endpoints θ0, θ1, θ2, …, θn, and equalwidth ∆θ.

Then, the rays θ = θi divide R into smallerregions withcentral angle ∆θ = θi – θi–1.

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AREAS IN POLAR COORDINATES

If we choose θi* in the i th subinterval [θi–1, θi] then the area ∆Ai of the i th region is the area of the sector of a circle with central angle ∆θand radius f(θ*).

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AREAS IN POLAR COORDINATES

Thus, from Formula 1, we have: ∆Ai ≈ ½[f(θi*)]2 ∆θ

So, an approximation to the total area A of R is:

* 212

1[ ( )]

n

ii

A f θ θ=

≈ ∆∑

Formula 2

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AREAS IN POLAR COORDINATES

It appears that the approximation in Formula 2 improves as n → ∞.

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AREAS IN POLAR COORDINATES

However, the sums in Formula 2 are Riemann sums for the function g(θ) = ½[f(θ)]2.

So, * 2 21 1

2 21

lim [ ( )] [ ( )]n b

i an if f dθ θ θ θ

→∞=

∆ =∑ ∫

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AREAS IN POLAR COORDINATES

Therefore, it appears plausible—and can, in fact, be proved—that the formula for the areaA of the polar region R is:

212 [ ( )]

b

aA f dθ θ= ∫

Formula 3

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AREAS IN POLAR COORDINATES

Formula 3 is often written as

with the understanding that r = f(θ).

Note the similarity between Formulas 1 and 4.

212

b

aA r dθ= ∫

Formula 4

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AREAS IN POLAR COORDINATES

When we apply Formula 3 or 4, it is helpful to think of the area as being swept out bya rotating ray through O that starts with angle a and ends with angle b.

Formula 4

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AREAS IN POLAR COORDINATES

Find the area enclosed by one loop of the four-leaved rose r = cos 2θ.

The curve r = cos 2θwas sketched in Example 8 in Section 10.3

Example 1

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AREAS IN POLAR COORDINATES

Notice that the region enclosed by the rightloop is swept out by a ray that rotates fromθ = –π/4 to θ = π/4.

Example 1

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AREAS IN POLAR COORDINATES

Hence, Formula 4 gives:

[ ]

4 2124

4 212 4

4 2

04

120

41 12 4 0

cos 2

cos 2

(1 cos 4 )

sin 48

A r d

d

d

d

π

π

π

π

π

π

π

θ

θ θ

θ θ

θ θ

πθ θ

=

=

=

= +

= + =

∫∫

Example 1

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AREAS IN POLAR COORDINATES

Find the area of the region that lies inside the circle r = 3 sin θ and outside the cardioid r = 1 + sin θ.

Example 2

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AREAS IN POLAR COORDINATES

The values of a and b in Formula 4 are determined by finding the points of intersection of the two curves.

Example 2

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AREAS IN POLAR COORDINATES

They intersect when 3 sin θ = 1 + sin θ, which gives sin θ = ½.

So, θ = π/6 and 5π/6.

Example 2

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AREAS IN POLAR COORDINATES

The desired area can be found by subtractingthe area inside the cardioid between θ = π/6 and θ = 5π/6 from the area inside the circlefrom π/6 to 5π/6.

Example 2

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AREAS IN POLAR COORDINATES

Thus,

5 6 212 6

5 6 212 6

(3sin )

(1 sin )

A d

d

π

π

π

π

θ θ

θ θ

=

− +

Example 2

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AREAS IN POLAR COORDINATES

As the region is symmetric about the vertical axis θ = π/2, we can write:

]

2 22 21 12 26 6

2 2

6

2 2 126

2

6

2 9sin (1 2sin sin )

(8sin 1 2sin )

(3 4cos 2 2sin ) assin (1 cos 2 )

3 2sin 2 2cos

A d d

d

d

π π

π π

π

π

π

π

π

π

θ θ θ θ θ

θ θ θ

θ θ θ θ

θ θ θ

π

= − + +

= − −

= − − = −

= − +

=

∫ ∫

Example 2

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AREAS IN POLAR COORDINATES

Example 2 illustrates the procedure for finding the area of the region bounded by two polar curves.

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AREAS IN POLAR COORDINATES

In general, let R be a region that is bounded by curves with polar equations

r = f(θ), r = g(θ), θ = a, θ = b,where: f(θ) ≥ g(θ) ≥ 0 0 < b – a < 2π

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AREAS IN POLAR COORDINATES

The area A of R is found by subtracting the area inside r = g(θ) from the area inside r = f(θ).

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AREAS IN POLAR COORDINATES

So, using Formula 3, we have:

( )

2 2

2 2

1 1[ ( )] [ ( )]2 2

1 [ ( )] [ ( )]2

θ θ θ θ

θ θ θ

= −

= −

∫ ∫

b b

a a

b

a

A f d g d

f g d

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CAUTION

The fact that a single point has manyrepresentations in polar coordinatessometimes makes it difficult to find all the points of intersection of two polar curves.

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CAUTION

For instance, it is obvious from this figure that the circle and the cardioid have threepoints of intersection.

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CAUTION

However, in Example 2, we solved the equations r = 3 sin θ and r = 1 + sin θand found only two such points:

(3/2, π/6) and (3/2, 5π/6)

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CAUTION

The origin is also a point of intersection.

However, we can’t find it by solving the equations of the curves.

The origin has no single representation in polar coordinates that satisfies both equations.

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CAUTION

Notice that, when represented as (0, 0) or (0, π), the origin satisfies r = 3 sin θ.

So, it lies on the circle.

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CAUTION

When represented as (0, 3 π/2), it satisfies r = 1 + sin θ.

So, it lies on the cardioid.

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CAUTION

Think of two points moving along the curves as the parameter value θincreases from 0 to 2π.

On one curve, the origin is reached at θ = 0 and θ = π.

On the other, it is reached at θ = 3π/2.

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CAUTION

The points don’t collide at the origin since they reach the origin at different times.

However, the curves intersect there nonetheless.

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CAUTION

Thus, to find all points of intersection of twopolar curves, it is recommended that youdraw the graphs of both curves.

It is especially convenient to use a graphing calculator or computer to help with this task.

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POINTS OF INTERSECTION

Find all points of intersection of the curves r = cos 2θ and r = ½.

If we solve the equations r = cos 2θ and r = ½, we get cos 2θ = ½.

Therefore, 2θ = π/3, 5π/3, 7π/3, 11π/3.

Example 3

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POINTS OF INTERSECTION

Thus, the values of θ between 0 and 2πthat satisfy both equations are:

θ = π/6, 5π/6, 7π/6, 11π/6

Example 3

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POINTS OF INTERSECTION

We have found four points of intersection:

(½, π/6), (½, 5π/6), (½, 7π/6), (½, 11π/6)

Example 3

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POINTS OF INTERSECTION

However, you can see that the curves have four other points of intersection:

(½, π/3), (½, 2π/3), (½, 4π/3), (½, 5π/3)

Example 3

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POINTS OF INTERSECTION

These can be found using symmetry or by noticing that another equation of the circle is r = -½.

Then, we solve r = cos 2θ and r = -½.

Example 3

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ARC LENGTH

To find the length of a polar curve r = f(θ), a ≤ θ ≤ b, we regard θ as a parameter andwrite the parametric equations of the curve as:

x = r cos θ = f(θ)cos θ

y = r sin θ = f (θ)sin θ

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ARC LENGTH

Using the Product Rule and differentiating with respect to θ, we obtain:

cos sin

sin cos

dx dr rd d

dy dr rd d

θ θθ θ

θ θθ θ

= −

= +

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ARC LENGTH

So, using cos2 θ + sin2 θ = 1,we have:2 2

22 2 2

22 2 2

22

cos 2 cos sin sin

sin 2 sin cos cos

dx dyd d

dr drr rd d

dr drr rd d

dr rd

θ θ

θ θ θ θθ θ

θ θ θ θθ θ

θ

+

= − +

+ + +

= +

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ARC LENGTH

Assuming that f’ is continuous, we can use Theorem 6 in Section 10.2 to write the arc length as:

2 2b

a

dx dyL dd d

θθ θ

= + ∫

Formula 5

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ARC LENGTH

Therefore, the length of a curve with polar equation r = f(θ), a ≤ θ ≤ b, is:

22b

a

drL r dd

θθ

= + ∫

Formula 5

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ARC LENGTH

Find the length of the cardioidr = 1 + sin θ

We sketched itin Example 7 in Section 10.3

Example 4

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ARC LENGTH

Its full length is given by the parameter interval0 ≤ θ ≤ 2π.

So, Formula 5 gives:2

2 2

0

2 2 2

02

0

(1 sin ) cos

2 2sin

drL r dd

d

d

π

π

π

θθ

θ θ θ

θ θ

= +

= + +

= +

∫∫

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ARC LENGTH

We could evaluate this integral by multiplying and dividing the integrand by or we could use a computer algebra system.

In any event, we find that the length of the cardioid is L = 8.

2 2sinθ−