Polar coordinates represent points in a plane using an ordered pair (r, θ) where r is the distance from a fixed point called the pole (or origin) and θ is the angle between the line from the pole to the point and a reference axis called the polar axis. Some key properties:
- Points (r, θ) and (-r, θ + π) represent the same location.
- Polar equations like r = a describe circles with radius a centered at the pole.
- Equations can be converted between Cartesian (x, y) and polar (r, θ) coordinates using trigonometric relationships.
- Graphs of polar equations r = f(θ) consist of all points satisfying
Introduction to polar coordinates and their representation in the plane and convenience compared to Cartesian coordinates.
Definition of polar coordinates involving the pole O, polar axis, distance r, and angle θ. Discusses the representation of points (r, θ) and negative r.
Examples of plotting specific points in polar coordinates, showcasing angles and quadrants where points are located.
Comparison between Cartesian and polar coordinates, highlighting representations and relationships between them.
Formulas connecting Cartesian and polar coordinates, including transformations and conversions between the systems.
Examples of converting points between Cartesian and polar coordinates, illustrating the non-uniqueness of θ in polar.
Introduction to polar curves defined by equations, with examples illustrating specific cases like circles and lines.
Detailed examples of plotting polar curves, including equations r = 2, circles, and visualization techniques.
Sketching more complex polar curves, identifying key points, symmetry, and loops formed by varying values of θ.
Finding tangent lines to polar curves, discussing horizontal and vertical tangents, and slope calculations.
Graphing techniques for polar curves, including the use of devices and parametric forms, with examples of limaçons.
Presentation of specific polar equations such as r = cos 3θ and r = 1 - cos θ.
A coordinate systemrepresents
a point in the plane by an ordered
pair of numbers called coordinates.
POLAR COORDINATES
3.
Usually, we useCartesian coordinates,
which are directed distances from two
perpendicular axes.
POLAR COORDINATES
4.
Here, we describea coordinate system
introduced by Newton, called the polar
coordinate system.
It is more convenient for many purposes.
POLAR COORDINATES
5.
Polar Coordinates
In thissection, we will learn:
How to represent points in polar coordinates.
POLAR COORDINATES
6.
POLE
We choose apoint in the plane
that is called the pole (or origin)
and is labeled O.
7.
POLAR AXIS
Then, wedraw a ray (half-line) starting
at O called the polar axis.
This axis is usually drawn horizontally to the right
corresponding to the positive x-axis in Cartesian
coordinates.
8.
ANOTHER POINT
If Pis any other point in the plane, let:
r be the distance from O to P.
θ be the angle (usually measured in radians)
between the polar axis and the line OP.
9.
POLAR COORDINATES
P isrepresented by the ordered pair (r, θ).
r, θ are called polar coordinates of P.
10.
POLAR COORDINATES
We usethe convention that
an angle is:
Positive—if measured in the counterclockwise
direction from the polar axis.
Negative—if measured in the clockwise
direction from the polar axis.
11.
If P =O, then r = 0, and we agree that
(0, θ) represents the pole for any value
of θ.
POLAR COORDINATES
12.
We extend themeaning of polar
coordinates (r, θ) to the case in which
r is negative—as follows.
POLAR COORDINATES
13.
POLAR COORDINATES
We agreethat, as shown, the points (–r, θ)
and (r, θ) lie on the same line through O
and at the same distance | r | from O, but
on opposite sides of O.
14.
POLAR COORDINATES
If r> 0, the point (r, θ) lies in the same
quadrant as θ.
If r < 0, it lies in the quadrant on the opposite
side of the pole.
Notice that (–r, θ)
represents
the same point
as (r, θ + π).
15.
POLAR COORDINATES
Plot thepoints whose polar coordinates
are given.
a. (1, 5π/4)
b. (2, 3π)
c. (2, –2π/3)
d. (–3, 3π/4)
Example 1
POLAR COORDINATES
The point(–3, 3π/4) is plotted.
It is is located three
units from the pole
in the fourth quadrant.
This is because
the angle 3π/4 is in
the second quadrant
and r = -3 is negative.
Example 1 d
20.
CARTESIAN VS. POLARCOORDINATES
In the Cartesian coordinate system, every
point has only one representation.
However, in the polar coordinate system,
each point has many representations.
21.
CARTESIAN VS. POLARCOORDINATES
For instance, the point (1, 5π/4) in
Example 1 a could be written as:
(1, –3π/4), (1, 13π/4), or (–1, π/4).
22.
CARTESIAN & POLARCOORDINATES
In fact, as a complete counterclockwise
rotation is given by an angle 2π, the point
represented by polar coordinates (r, θ) is
also represented by
(r, θ + 2nπ) and (-r, θ + (2n + 1)π)
where n is any integer.
23.
CARTESIAN & POLARCOORDINATES
The connection between polar and Cartesian
coordinates can be seen here.
The pole corresponds to the origin.
The polar axis coincides with the positive x-axis.
24.
CARTESIAN & POLARCOORDINATES
If the point P has Cartesian coordinates (x, y)
and polar coordinates (r, θ), then, from
the figure, we have: cos sin
x y
r r
θ θ= =
CARTESIAN & POLARCOORDS.
Although Equations 1 were deduced from
the figure (which illustrates the case where
r > 0 and 0 < θ < π/2), these equations are
valid for all values of r and θ.
See the general
definition of sin θ
and cos θ
in Appendix D.
27.
CARTESIAN & POLARCOORDS.
Equations 1 allow us to find
the Cartesian coordinates of a point
when the polar coordinates are known.
28.
CARTESIAN & POLARCOORDS.
To find r and θ when x and y are known,
we use the equations
These can be
deduced from
Equations 1 or
simply read from
the figure.
2 2 2
tan
y
r x y
x
θ= + =
Equations 2
29.
CARTESIAN & POLARCOORDS.
Convert the point (2, π/3) from polar to
Cartesian coordinates.
Since r = 2 and θ = π/3,
Equations 1 give:
Thus, the point is (1, ) in Cartesian coordinates.
Example 2
1
cos 2cos 2 1
3 2
3
sin 2sin 2. 3
3 2
x r
y r
π
θ
π
θ
= = = × =
= = = =
3
30.
CARTESIAN & POLARCOORDS.
Represent the point with Cartesian
coordinates (1, –1) in terms of polar
coordinates.
Example 3
31.
CARTESIAN & POLARCOORDS.
If we choose r to be positive, then
Equations 2 give:
As the point (1, –1) lies in the fourth quadrant,
we can choose θ = –π/4 or θ = 7π/4.
Example 3
2 2 2 2
1 ( 1) 2
tan 1
r x y
y
x
θ
= + = + − =
= = −
32.
CARTESIAN & POLARCOORDS.
Thus, one possible answer is:
( , –π/4)
Another possible answer is:
( , 7π/4)
Example 3
2
2
33.
CARTESIAN & POLARCOORDS.
Equations 2 do not uniquely determine θ
when x and y are given.
This is because, as θ increases through the interval
0 ≤ θ ≤ 2π, each value of tan θ occurs twice.
Note
34.
CARTESIAN & POLARCOORDS.
So, in converting from Cartesian to polar
coordinates, it’s not good enough just to find r
and θ that satisfy Equations 2.
As in Example 3, we must choose θ so that
the point (r, θ) lies in the correct quadrant.
Note
35.
POLAR CURVES
The graphof a polar equation r = f(θ)
[or, more generally, F(r, θ) = 0] consists
of all points that have at least one polar
representation (r, θ), whose coordinates
satisfy the equation.
36.
POLAR CURVES
What curveis represented by
the polar equation r = 2 ?
The curve consists of all points (r, θ)
with r = 2.
r represents the distance from the point
to the pole.
Example 4
37.
POLAR CURVES
Thus,the curve r = 2 represents
the circle with center O and radius 2.
Example 4
38.
POLAR CURVES
In general,the equation r = a represents
a circle O with center and radius |a|.
Example 4
39.
POLAR CURVES
Sketch thepolar curve θ = 1.
This curve consists of all points (r, θ)
such that the polar angle θ is 1 radian.
Example 5
40.
POLAR CURVES
It isthe straight line that passes through O
and makes an angle of 1 radian with the polar
axis.
Example 5
41.
POLAR CURVES
Notice that:
The points (r, 1) on
the line with r > 0 are
in the first quadrant.
The points (r, 1) on
the line with r < 0 are
in the third quadrant.
Example 5
42.
POLAR CURVES
a. Sketchthe curve with polar equation
r = 2 cos θ.
b. Find a Cartesian equation for this curve.
Example 6
POLAR CURVES
We haveused only values of θ between 0
and π—since, if we let θ increase beyond π,
we obtain the same points again.
Example 6 a
47.
POLAR CURVES
To convertthe given equation to a Cartesian
equation, we use Equations 1 and 2.
From x = r cos θ, we have cos θ = x/r.
So, the equation r = 2 cos θ becomes r = 2x/r.
This gives:
2x = r2
= x2
+ y2
or x2
+ y2
– 2x = 0
Example 6 b
48.
POLAR CURVES
Completing thesquare,
we obtain:
(x – 1)2
+ y2
= 1
The equation is of a circle with center (1, 0)
and radius 1.
Example 6 b
49.
POLAR CURVES
The figureshows a geometrical illustration
that the circle in Example 6 has the equation
r = 2 cos θ.
The angle OPQ is
a right angle,
and so r/2 = cos θ.
Why is OPQ
a right angle?
50.
POLAR CURVES
Sketch thecurve r = 1 + sin θ.
Here, we do not plot points as in Example 6.
Rather, we first sketch the graph of r = 1 + sin θ
in Cartesian coordinates by shifting the sine curve
up one unit—as follows.
Example 7
51.
POLAR CURVES
This enablesus to read at a glance the
values of r that correspond to increasing
values of θ.
Example 7
52.
POLAR CURVES
For instance,we see that, as θ increases
from 0 to π/2, r (the distance from O)
increases from 1 to 2.
Example 7
53.
POLAR CURVES
So, wesketch the corresponding part
of the polar curve.
Example 7
54.
POLAR CURVES
As θincreases from π/2 to π,
the figure shows that r decreases
from 2 to 1.
Example 7
POLAR CURVES
Sketch thecurve r = cos 2θ.
As in Example 7, we first sketch r = cos 2θ,
0 ≤ θ ≤2π, in Cartesian coordinates.
Example 8
62.
POLAR CURVES
As θincreases from 0 to π/4,
the figure shows that r decreases
from 1 to 0.
Example 8
63.
POLAR CURVES
So, wedraw the
corresponding portion
of the polar curve
(indicated by ).1
Example 8
64.
POLAR CURVES
As θincreases from π/4 to π/2, r goes
from 0 to –1.
This means that the distance from O increases
from 0 to 1.
Example 8
65.
POLAR CURVES
However,instead of being
in the first quadrant,
this portion of the polar curve
(indicated by ) lies on
the opposite side of the pole
in the third quadrant.
2
Example 8
66.
POLAR CURVES
The restof the curve is
drawn in a similar fashion.
The arrows and numbers
indicate the order in which
the portions are traced out.
Example 8
RULE 1
If apolar equation is unchanged when θ
is replaced by –θ, the curve is symmetric
about the polar axis.
71.
RULE 2
If theequation is unchanged when r is
replaced by –r, or when θ is replaced by
θ + π, the curve is symmetric about the pole.
This means that
the curve remains
unchanged if we rotate
it through 180° about
the origin.
72.
RULE 3
If theequation is unchanged when θ is
replaced by π – θ, the curve is symmetric
about the vertical line θ = π/2.
SYMMETRY
For instance, inExample 6, we need only
have plotted points for 0 ≤ θ ≤ π/2 and then
reflected about the polar axis to obtain
the complete circle.
78.
TANGENTS TO POLARCURVES
To find a tangent line to a polar curve r = f(θ),
we regard θ as a parameter and write its
parametric equations as:
x = r cos θ = f (θ) cos θ
y = r sin θ = f (θ) sin θ
79.
TANGENTS TO POLARCURVES
Then, using the method for finding slopes of
parametric curves (Equation 2 in Section 10.2)
and the Product Rule, we have:
Equation 3
sin cos
cos sin
dy dr
r
dy d d
dx drdx r
d d
θ θ
θ θ
θ θ
θ θ
+
= =
−
80.
TANGENTS TO POLARCURVES
We locate horizontal tangents by finding
the points where dy/dθ = 0 (provided that
dx/dθ ≠ 0).
Likewise, we locate vertical tangents at
the points where dx/dθ = 0 (provided that
dy/dθ ≠ 0).
81.
TANGENTS TO POLARCURVES
Notice that, if we are looking for tangent
lines at the pole, then r = 0 and Equation 3
simplifies to:
tan if 0
dy dr
dx d
θ
θ
= ≠
82.
TANGENTS TO POLARCURVES
For instance, in Example 8, we found that
r = cos 2θ = 0 when θ = π/4 or 3π/4.
This means that the lines θ = π/4 and θ = 3π/4
(or y = x and y = –x) are tangent lines to r = cos 2θ
at the origin.
83.
TANGENTS TO POLARCURVES
a. For the cardioid r = 1 + sin θ of Example 7,
find the slope of the tangent line when
θ = π/3.
b. Find the points on the cardioid where
the tangent line is horizontal or vertical.
Example 9
84.
TANGENTS TO POLARCURVES
Using Equation 3 with r = 1 + sin θ, we have:
2
sin cos
cos sin
cos sin (1 sin )cos
cos cos (1 sin )sin
cos (1 2sin ) cos (1 2sin )
1 2sin sin (1 sin )(1 2sin )
dr
r
dy d
drdx r
d
θ θ
θ
θ θ
θ
θ θ θ θ
θ θ θ θ
θ θ θ θ
θ θ θ θ
+
=
−
+ +
=
− +
+ +
= =
− − + −
Example 9
85.
TANGENTS TO POLARCURVES
The slope of the tangent at the point where
θ = π/3 is:
Example 9 a
3
1
2
cos( /3)(1 2sin( /3))
(1 sin( /3))(1 2sin( /3)
(1 3)
(1 3 / 2)(1 3)
1 3 1 3
1
(2 3)(1 3) 1 3
dy
dx θ π
π π
π π=
+
=
+ −
+
=
+ −
+ +
= = = −
+ − − −
TANGENTS TO POLARCURVES
Hence, there are horizontal tangents at
the points
(2, π/2), (½, 7π/6), (½, 11π/6)
and vertical tangents at
(3/2, π/6), (3/2, 5π/6)
When θ = 3π/2, both dy/dθ and dx/dθ are 0.
So, we must be careful.
Example 9 b
88.
TANGENTS TO POLARCURVES
Using l’Hospital’s Rule, we have:
(3 / 2)
(3 / 2) (3 / 2)
(3 /2)
(3 /2)
lim
1 2sin cos
lim lim
1 2sin 1 sin
1 cos
lim
3 1 sin
1 sin
lim
3 cos
dy
dxθ π
θ π θ π
θ π
θ π
θ θ
θ θ
θ
θ
θ
θ
−
− −
−
−
→
→ →
→
→
+
= ÷ ÷
− +
= −
+
−
= − = ∞
Example 9 b
89.
TANGENTS TO POLARCURVES
By symmetry,
(3 / 2)
lim
dy
dxθ π +
→
= −∞
Example 9 b
90.
TANGENTS TO POLARCURVES
Thus, there is a vertical tangent line
at the pole.
Example 9 b
91.
TANGENTS TO POLARCURVES
Instead of having to remember Equation 3,
we could employ the method used to
derive it.
For instance, in Example 9, we could have written:
x = r cos θ = (1 + sin θ) cos θ = cos θ + ½ sin 2θ
y = r sin θ = (1 + sin θ) sin θ = sin θ + sin2
θ
Note
92.
TANGENTS TO POLARCURVES
Then, we would have
which is equivalent to our previous
expression.
Note
/ cos 2sin cos
/ sin cos2
cos sin 2
sin cos2
dy dy d
dx dx d
θ θ θ θ
θ θ θ
θ θ
θ θ
+
= =
− +
+
=
− +
GRAPHING POLAR CURVES
However,we need to use a graphing
calculator or computer when faced with curves
as complicated as shown.
95.
GRAPHING POLAR CURVESWITH GRAPHING DEVICES
Some graphing devices have commands that
enable us to graph polar curves directly.
With other machines, we need to convert to
parametric equations first.
96.
GRAPHING WITH DEVICES
Inthis case, we take the polar equation r = f(θ)
and write its parametric equations as:
x = r cos θ = f(θ) cos θ
y = r sin θ = f(θ) sin θ
Some machines require that the parameter
be called t rather than θ.
97.
GRAPHING WITH DEVICES
Graphthe curve r = sin(8θ / 5).
Let’s assume that our graphing device doesn’t
have a built-in polar graphing command.
Example 10
98.
GRAPHING WITH DEVICES
Inthis case, we need to work with
the corresponding parametric equations,
which are:
In any case, we need to determine
the domain for θ.
Example 10
cos sin(8 /5)cos
sin sin(8 /5)sin
x r
y r
θ θ θ
θ θ θ
= =
= =
99.
GRAPHING WITH DEVICES
So,we ask ourselves:
How many complete rotations are required
until the curve starts to repeat itself ?
Example 10
100.
GRAPHING WITH DEVICES
Ifthe answer is n, then
So, we require that 16nπ/5
be an even multiple of π.
8( 2 ) 8 16
sin sin
5 5 5
8
sin
5
n nθ π θ π
θ
+
= + ÷
=
Example 10
101.
GRAPHING WITH DEVICES
Thiswill first occur when n = 5.
Hence, we will graph the entire curve
if we specify that 0 ≤ θ ≤ 10π.
Example 10
102.
GRAPHING WITH DEVICES
Switchingfrom θ to t,
we have the equations
sin(8 /5)cos
sin(8 /5)sin
0 10
x t t
y t t
t π
=
=
≤ ≤
Example 10
GRAPHING WITH DEVICES
Investigatethe family of polar curves given
by r = 1 + c sin θ.
How does the shape change as c changes?
These curves are called limaçons—after a French word
for snail, because of the shape of the curves for certain
values of c.
Example 11