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Conic Sections in Polar Coordinates

Conic Sections in Polar Coordinates

By the end of this section, you will be able to:

  • Identify a conic in polar form
  • Graph the polar equations of conics
  • Define conics in terms of a focus and a directrix

Most of us are familiar with orbital motion, such as the motion of a planet around the sun or an electron around an atomic nucleus. Within the planetary system, orbits of planets, asteroids, and comets around a larger celestial body are often elliptical. Comets, however, may take on a parabolic or hyperbolic orbit instead. And, in reality, the characteristics of the planets’ orbits may vary over time. Each orbit is tied to the location of the celestial body being orbited and the distance and direction of the planet or other object from that body. As a result, we tend to use polar coordinates to represent these orbits.

In an elliptical orbit, the periapsis is the point at which the two objects are closest, and the apoapsis is the point at which they are farthest apart. Generally, the velocity of the orbiting body tends to increase as it approaches the periapsis and decrease as it approaches the apoapsis. Some objects reach an escape velocity, which results in an infinite orbit. These bodies exhibit either a parabolic or a hyperbolic orbit about a body; the orbiting body breaks free of the celestial body’s gravitational pull and fires off into space. Each of these orbits can be modeled by a conic section in the polar coordinate system.

Identifying a Conic in Polar Form

Any conic may be determined by three characteristics: a single focus, a fixed line called the directrix, and the ratio of the distances of each to a point on the graph. Consider the parabola shown below, whose focus is at the pole.

In The Parabola, we learned how a parabola is defined by the focus (a fixed point) and the directrix (a fixed line). In this section, we will learn how to define any conic in the polar coordinate system in terms of a fixed point, the focus P(r,θ)P(r,\theta) at the pole, and a line, the directrix, which is perpendicular to the polar axis.

If FF is a fixed point, the focus, and DD is a fixed line, the directrix, then we can let ee be a fixed positive number, called the eccentricity, which we can define as the ratio of the distances from a point on the graph to the focus and the point on the graph to the directrix. Then the set of all points PP such that e=PFPDe=\tfrac{PF}{PD} is a conic. In other words, we can define a conic as the set of all points PP with the property that the ratio of the distance from PP to FF to the distance from PP to DD is equal to the constant ee.

For a conic with eccentricity ee,

  • if 0e<10\le e<1, the conic is an ellipse
  • if e=1e=1, the conic is a parabola
  • if e>1e>1, the conic is a hyperbola

With this definition, we may now define a conic in terms of the directrix, x=±px=\pm p, the eccentricity ee, and the angle θ\theta. Thus, each conic may be written as a polar equation, an equation written in terms of rr and θ\theta.

The Polar Equation for a Conic. For a conic with a focus at the origin, if the directrix is x=±px=\pm p, where pp is a positive real number, and the eccentricity is a positive real number ee, the conic has a polar equation

r=ep1±ecosθr=\tfrac{ep}{1\pm e\cos\theta}

For a conic with a focus at the origin, if the directrix is y=±py=\pm p, where pp is a positive real number, and the eccentricity is a positive real number ee, the conic has a polar equation

r=ep1±esinθr=\tfrac{ep}{1\pm e\sin\theta}

How To: given the polar equation for a conic, identify the type of conic, the directrix, and the eccentricity.

  1. Multiply the numerator and denominator by the reciprocal of the constant in the denominator to rewrite the equation in standard form.
  2. Identify the eccentricity ee as the coefficient of the trigonometric function in the denominator.
  3. Compare ee with 11 to determine the shape of the conic.
  4. Determine the directrix as x=px=p if cosine is in the denominator and y=py=p if sine is in the denominator. Set epep equal to the numerator in standard form to solve for xx or yy.

Example. For each of the following equations, identify the conic with focus at the origin, the directrix, and the eccentricity.

a. r=63+2sinθr=\tfrac{6}{3+2\sin\theta} b. r=124+5cosθr=\tfrac{12}{4+5\cos\theta} c. r=722sinθr=\tfrac{7}{2-2\sin\theta}

Solution. For each of the three conics, we will rewrite the equation in standard form. Standard form has a 11 as the constant in the denominator. Therefore, in all three parts, the first step will be to multiply the numerator and denominator by the reciprocal of the constant of the original equation, 1c\tfrac1c, where cc is that constant.

a. Multiply the numerator and denominator by 13\tfrac13.

r=63+2sinθ(13)(13)=6(13)3(13)+2(13)sinθ=21+23sinθr=\tfrac{6}{3+2\sin\theta}\cdot\tfrac{\left(\tfrac13\right)}{\left(\tfrac13\right)}=\tfrac{6\left(\tfrac13\right)}{3\left(\tfrac13\right)+2\left(\tfrac13\right)\sin\theta}=\tfrac{2}{1+\tfrac23\sin\theta}

Because sinθ\sin\theta is in the denominator, the directrix is y=py=p. Comparing to standard form, note that e=23e=\tfrac23. Therefore, from the numerator,

2=ep2=23p(32)2=(32)23p3=p \begin{array}{lrcl} & 2 &=& ep \\[4pt] & 2 &=& \tfrac23p \\[4pt] & \left(\tfrac32\right)2 &=& \left(\tfrac32\right)\tfrac23p \\[4pt] & 3 &=& p \end{array}

Since e<1e<1, the conic is an ellipse. The eccentricity is e=23e=\tfrac23 and the directrix is y=3y=3.

b. Multiply the numerator and denominator by 14\tfrac14.

r=124+5cosθ(14)(14)=12(14)4(14)+5(14)cosθ=31+54cosθr=\tfrac{12}{4+5\cos\theta}\cdot\tfrac{\left(\tfrac14\right)}{\left(\tfrac14\right)}=\tfrac{12\left(\tfrac14\right)}{4\left(\tfrac14\right)+5\left(\tfrac14\right)\cos\theta}=\tfrac{3}{1+\tfrac54\cos\theta}

Because cosθ\cos\theta is in the denominator, the directrix is x=px=p. Comparing to standard form, e=54e=\tfrac54. Therefore, from the numerator,

3=ep3=54p(45)3=(45)54p125=p \begin{array}{lrcl} & 3 &=& ep \\[4pt] & 3 &=& \tfrac54p \\[4pt] & \left(\tfrac45\right)3 &=& \left(\tfrac45\right)\tfrac54p \\[4pt] & \tfrac{12}{5} &=& p \end{array}

Since e>1e>1, the conic is a hyperbola. The eccentricity is e=54e=\tfrac54 and the directrix is x=125=2.4x=\tfrac{12}{5}=2.4.

c. Multiply the numerator and denominator by 12\tfrac12.

r=722sinθ(12)(12)=7(12)2(12)2(12)sinθ=721sinθr=\tfrac{7}{2-2\sin\theta}\cdot\tfrac{\left(\tfrac12\right)}{\left(\tfrac12\right)}=\tfrac{7\left(\tfrac12\right)}{2\left(\tfrac12\right)-2\left(\tfrac12\right)\sin\theta}=\tfrac{\tfrac72}{1-\sin\theta}

Because sine is in the denominator, the directrix is y=py=-p. Comparing to standard form, e=1e=1. Therefore, from the numerator,

72=ep72=(1)p72=p \begin{array}{lrcl} & \tfrac72 &=& ep \\[4pt] & \tfrac72 &=& (1)p \\[4pt] & \tfrac72 &=& p \end{array}

Because e=1e=1, the conic is a parabola. The eccentricity is e=1e=1 and the directrix is y=72=3.5y=-\tfrac72=-3.5.

Identify the conic with focus at the origin forr=23cosθr=\tfrac{2}{3-\cos\theta}.

Find the eccentricityeeof the conicr=23cosθr=\tfrac{2}{3-\cos\theta}.

Find the directrix, as an equation, of the conicr=23cosθr=\tfrac{2}{3-\cos\theta}.

Graphing the Polar Equations of Conics

When graphing in Cartesian coordinates, each conic section has a unique equation. This is not the case when graphing in polar coordinates. We must use the eccentricity of a conic section to determine which type of curve to graph, and then determine its specific characteristics. The first step is to rewrite the conic in standard form as we have done in the previous example. In other words, we need to rewrite the equation so that the denominator begins with 11. This enables us to determine ee and, therefore, the shape of the curve. The next step is to substitute values for θ\theta and solve for rr to plot a few key points. Setting θ\theta equal to 0,π2,π,0,\tfrac{\pi}{2},\pi, and 3π2\tfrac{3\pi}{2} provides the vertices so we can create a rough sketch of the graph.

Example. Graph r=53+3cosθr=\tfrac{5}{3+3\cos\theta}.

Solution. First, we rewrite the conic in standard form by multiplying the numerator and denominator by the reciprocal of 33, which is 13\tfrac13.

r=53+3cosθ=5(13)3(13)+3(13)cosθ=531+cosθr=\tfrac{5}{3+3\cos\theta}=\tfrac{5\left(\tfrac13\right)}{3\left(\tfrac13\right)+3\left(\tfrac13\right)\cos\theta}=\tfrac{\tfrac53}{1+\cos\theta}

Because e=1e=1, we will graph a parabola with a focus at the origin. The function has a cosθ\cos\theta, and there is an addition sign in the denominator, so the directrix is x=px=p.

53=ep53=(1)p53=p \begin{array}{lrcl} & \tfrac53 &=& ep \\[4pt] & \tfrac53 &=& (1)p \\[4pt] & \tfrac53 &=& p \end{array}

The directrix is x=53x=\tfrac53.

Plotting a few key points as in the table below will enable us to see the vertices. See the figure below.

ABCD
θ\theta00π2\tfrac{\pi}{2}π\pi3π2\tfrac{3\pi}{2}
r=53+3cosθr=\tfrac{5}{3+3\cos\theta}560.83\tfrac56\approx0.83531.67\tfrac53\approx1.67undefined531.67\tfrac53\approx1.67

Analysis. We can check our result with a graphing utility. See the figure below.

Example. Graph r=823sinθr=\tfrac{8}{2-3\sin\theta}.

Solution. First, we rewrite the conic in standard form by multiplying the numerator and denominator by the reciprocal of 22, which is 12\tfrac12.

r=823sinθ=8(12)2(12)3(12)sinθ=4132sinθr=\tfrac{8}{2-3\sin\theta}=\tfrac{8\left(\tfrac12\right)}{2\left(\tfrac12\right)-3\left(\tfrac12\right)\sin\theta}=\tfrac{4}{1-\tfrac32\sin\theta}

Because e=32,e>1e=\tfrac32,e>1, so we will graph a hyperbola with a focus at the origin. The function has a sinθ\sin\theta term and there is a subtraction sign in the denominator, so the directrix is y=py=-p.

4=ep4=(32)p4(23)=p83=p \begin{array}{lrcl} & 4 &=& ep \\[4pt] & 4 &=& \left(\tfrac32\right)p \\[4pt] & 4\left(\tfrac23\right) &=& p \\[4pt] & \tfrac83 &=& p \end{array}

The directrix is y=83y=-\tfrac83.

Plotting a few key points as in the table below will enable us to see the vertices. See the figure below.

ABCD
θ\theta00π2\tfrac{\pi}{2}π\pi3π2\tfrac{3\pi}{2}
r=823sinθr=\tfrac{8}{2-3\sin\theta}448-84485=1.6\tfrac85=1.6

Example. Graph r=1054cosθr=\tfrac{10}{5-4\cos\theta}.

Solution. First, we rewrite the conic in standard form by multiplying the numerator and denominator by the reciprocal of 55, which is 15\tfrac15.

r=1054cosθ=10(15)5(15)4(15)cosθ=2145cosθr=\tfrac{10}{5-4\cos\theta}=\tfrac{10\left(\tfrac15\right)}{5\left(\tfrac15\right)-4\left(\tfrac15\right)\cos\theta}=\tfrac{2}{1-\tfrac45\cos\theta}

Because e=45,e<1e=\tfrac45,e<1, so we will graph an ellipse with a focus at the origin. The function has a cosθ\cos\theta, and there is a subtraction sign in the denominator, so the directrix is x=px=-p.

2=ep2=(45)p2(54)=p52=p \begin{array}{lrcl} & 2 &=& ep \\[4pt] & 2 &=& \left(\tfrac45\right)p \\[4pt] & 2\left(\tfrac54\right) &=& p \\[4pt] & \tfrac52 &=& p \end{array}

The directrix is x=52x=-\tfrac52.

Plotting a few key points as in the table below will enable us to see the vertices. See the figure below.

ABCD
θ\theta00π2\tfrac{\pi}{2}π\pi3π2\tfrac{3\pi}{2}
r=1054cosθr=\tfrac{10}{5-4\cos\theta}1010221091.1\tfrac{10}{9}\approx1.122

Analysis. We can check our result using a graphing utility. See the figure below.

Which graph showsr=24cosθr=\tfrac{2}{4-\cos\theta}?

Defining Conics in Terms of a Focus and a Directrix

So far we have been using polar equations of conics to describe and graph the curve. Now we will work in reverse; we will use information about the origin, eccentricity, and directrix to determine the polar equation.

How To: given the focus, eccentricity, and directrix of a conic, determine the polar equation.

  1. Determine whether the directrix is horizontal or vertical. If the directrix is given in terms of yy, we use the general polar form in terms of sine. If the directrix is given in terms of xx, we use the general polar form in terms of cosine.
  2. Determine the sign in the denominator. If p<0p<0, use subtraction. If p>0p>0, use addition.
  3. Write the coefficient of the trigonometric function as the given eccentricity.
  4. Write the absolute value of pp in the numerator, and simplify the equation.

Example. Find the polar form of the conic given a focus at the origin, e=3e=3, and directrix y=2y=-2.

Solution. The directrix is y=py=-p, so we know the trigonometric function in the denominator is sine.

Because y=2,2<0y=-2,-2<0, so we know there is a subtraction sign in the denominator. We use the standard form of

r=ep1esinθr=\tfrac{ep}{1-e\sin\theta}

and e=3e=3 and 2=2=p|-2|=2=p.

Therefore,

r=(3)(2)13sinθr=613sinθ \begin{array}{lrcl} & r &=& \tfrac{(3)(2)}{1-3\sin\theta} \\[4pt] & r &=& \tfrac{6}{1-3\sin\theta} \end{array}

Example. Find the polar form of a conic given a focus at the origin, e=35e=\tfrac35, and directrix x=4x=4.

Solution. Because the directrix is x=px=p, we know the function in the denominator is cosine. Because x=4,4>0x=4,4>0, so we know there is an addition sign in the denominator. We use the standard form of

r=ep1+ecosθr=\tfrac{ep}{1+e\cos\theta}

and e=35e=\tfrac35 and 4=4=p|4|=4=p.

Therefore,

r=(35)(4)1+35cosθr=1251+35cosθr=1251(55)+35cosθr=12555+35cosθr=12555+3cosθr=125+3cosθ \begin{array}{lrcl} & r &=& \tfrac{\left(\tfrac35\right)(4)}{1+\tfrac35\cos\theta} \\[4pt] & r &=& \tfrac{\tfrac{12}{5}}{1+\tfrac35\cos\theta} \\[4pt] & r &=& \tfrac{\tfrac{12}{5}}{1\left(\tfrac55\right)+\tfrac35\cos\theta} \\[4pt] & r &=& \tfrac{\tfrac{12}{5}}{\tfrac55+\tfrac35\cos\theta} \\[4pt] & r &=& \tfrac{12}{5}\cdot\tfrac{5}{5+3\cos\theta} \\[4pt] & r &=& \tfrac{12}{5+3\cos\theta} \end{array}

Find the polar form of the conic given a focus at the origin,e=1e=1, and directrixx=1x=-1.

Example. Convert the conic r=155sinθr=\tfrac{1}{5-5\sin\theta} to rectangular form.

Solution. We will rearrange the formula to use the identities r=x2+y2,x=rcosθ,r=\sqrt{x^2+y^2},x=r\cos\theta, and y=rsinθy=r\sin\theta.

r=155sinθEliminate the fraction.r(55sinθ)=1Distribute.5r5rsinθ=1Isolate 5r.5r=1+5rsinθSquare both sides.25r2=(1+5rsinθ)2Substitute r=x2+y2 and y=rsinθ.25(x2+y2)=(1+5y)2Distribute and use FOIL.25x2+25y2=1+10y+25y2Rearrange terms and set equal to 1.25x210y=1 \begin{array}{lrcl} & r &=& \tfrac{1}{5-5\sin\theta} \\[4pt] \text{Eliminate the fraction.} & r(5-5\sin\theta) &=& 1 \\[4pt] \text{Distribute.} & 5r-5r\sin\theta &=& 1 \\[4pt] \text{Isolate }5r. & 5r &=& 1+5r\sin\theta \\[4pt] \text{Square both sides.} & 25r^2 &=& (1+5r\sin\theta)^2 \\[4pt] \text{Substitute }r=\sqrt{x^2+y^2}\text{ and }y=r\sin\theta. & 25(x^2+y^2) &=& (1+5y)^2 \\[4pt] \text{Distribute and use FOIL.} & 25x^2+25y^2 &=& 1+10y+25y^2 \\[4pt] \text{Rearrange terms and set equal to 1.} & 25x^2-10y &=& 1 \end{array}

Convert the conicr=21+2cosθr=\tfrac{2}{1+2\cos\theta}to rectangular form.

Media. Access these online resources for additional instruction and practice with conics in polar coordinates.

Key concepts

  • Any conic may be determined by a single focus, the corresponding eccentricity, and the directrix. We can also define a conic in terms of a fixed point, the focus P(r,θ)P(r,\theta) at the pole, and a line, the directrix, which is perpendicular to the polar axis.
  • A conic is the set of all points e=PFPDe=\tfrac{PF}{PD}, where eccentricity ee is a positive real number. Each conic may be written in terms of its polar equation.
  • The polar equations of conics can be graphed.
  • Conics can be defined in terms of a focus, a directrix, and eccentricity.
  • We can use the identities r=x2+y2,x=rcosθ,r=\sqrt{x^2+y^2},x=r\cos\theta, and y=rsinθy=r\sin\theta to convert the equation for a conic from polar to rectangular form.

Practice

Identify a conic in polar form

Identify the conic with focus at the origin forr(7+8cosθ)=7r(7+8\cos\theta)=7.

Find the eccentricityeeof the conicr=47+2cosθr=\tfrac{4}{7+2\cos\theta}.

Find the directrix, as an equation, of the conicr=51+2sinθr=\tfrac{5}{1+2\sin\theta}.

Graph the polar equations of conics

The conicr(1+cosθ)=5r(1+\cos\theta)=5is a parabola with focus at the origin. Give its vertex as an ordered pair(x,y)(x,y).

The conicr=1054sinθr=\tfrac{10}{5-4\sin\theta}is an ellipse with focus at the origin. Give both vertices, as ordered pairs separated by a comma.

Which graph showsr=845cosθr=\tfrac{8}{4-5\cos\theta}?

Define conics in terms of a focus and a directrix

Find the polar equation of the conic with focus at the origin, directrixx=1x=1, and eccentricitye=1e=1.

Find the polar equation of the conic with focus at the origin, directrixy=4y=4, and eccentricitye=32e=\tfrac32.

Convert the polar equationr(2cosθ)=1r(2-\cos\theta)=1to rectangular form.


This section is adapted from Precalculus 2e, Section 10.5: Conic Sections in Polar Coordinates by Jay Abramson and OpenStax, © OpenStax, licensed under CC BY-NC-SA 4.0. Access the original for free at openstax.org. Changes: this module (unlike m49438–m49441 earlier in the chapter) carries no coreq-skills prelude, and its own Section Exercises are followed by the chapter’s Review Exercises and Practice Test appended in the same file; those chapter-level exercises were not transcribed and no Practice item was drawn from them. Omitted the credit photograph of the solar system (NASA Blueshift, Flickr), keeping the two paragraphs that introduce it. Kept the Media callout’s introductory sentence but omitted its three external video links, matching house precedent elsewhere in this book. Recreated all six instructional figures as accessible spec-first SVGs on ordinary Cartesian axes with tick labels, rather than the source’s polar-grid background of concentric circles and radial spokes — matching this book’s own §8.4 convention for polar-equation graphs, since the figure engine has no polar-grid primitive: the introductory focus/directrix/angle schematic, drawn as the exact parabola r=21cosθr=\tfrac{2}{1-\cos\theta} (focus at the pole, directrix x=2x=-2, a point PP at θ=70\theta=70^\circ with its equal distances to the focus and to the directrix marked) — the source labels its figure x=2+y2x=2+y^2 while placing the focus at the pole, which that parabola’s focus (94,0)(\tfrac94,0) is not, so the local figure and the sentence introducing it name no equation other than the polar one it actually plots (a source defect, logged in the errata); the three worked-example graphs (a parabola, a hyperbola, and an ellipse), each sampled as polylines from the exact equation with points A–D placed at the printed table’s θ=0,π2,π,3π2\theta=0,\tfrac{\pi}{2},\pi,\tfrac{3\pi}{2} values and the hyperbola’s two branches split where the denominator changes sign; and the two “Analysis” graphing-utility check figures (bare re-renders of the same two curves, unlabeled, matching the source’s own unlabeled check art). The grader proves two polar equations of the same conic equal, so “find the polar equation” answers carry no answerForm — a printed-subject retype is not a hazard here because the prompt states only the focus, eccentricity, and directrix in prose, never an equation to retype — and are keyed in whichever of the standard or fraction-cleared integer form the source itself prints. Every “identify the conic” ask is a multiplechoice over ellipse/parabola/hyperbola; eccentricity is keyed as a bare number or fraction, never the letter ee; a directrix is keyed as an equation (x=2x=-2, y=52y=\tfrac52) with the question saying “as an equation.” The module’s second in-page Try It (“Graph r=24cosθr=\tfrac{2}{4-\cos\theta}”, solution a figure only) is a graph-mode multiple choice over four spec-first options that vary orientation, mirror sign, and eccentricity — following the 9.3 precedent — since the grader cannot take a drawn curve as a submitted answer; the section’s other in-page Try Its keep their source form (identify/eccentricity/directrix fill-ins and multiple choice, or a safe polar-to-rectangular re-expression fill-in). In the closing Practice block, three end-of-section “graph the conic” exercises (Algebraic #39, #33, and #35 in this book’s local numbering, for the vertex, both-vertices, and graph-recognition items respectively) are likewise adapted into a computed fill-in on the vertex or vertices the sketch needs, or a graph-recognition multiple choice, each appearing once (not duplicated with the in-page set). Nine selected end-of-section Algebraic exercises were adapted into the interactive components of the closing Practice block, one Practice group per objective, every one independently re-derived — including by running the arithmetic in Node — rather than read off the source key. One suspected source defect (Algebraic #55: directrix x=3,e=13x=-3,e=\tfrac13) prints a key, r=333cosθr=\tfrac{3}{3-3\cos\theta}, that simplifies to e=1e=1 and contradicts its own stated eccentricity of 13\tfrac13; the correctly derived r=33cosθr=\tfrac{3}{3-\cos\theta} was independently verified but the exercise itself was not used on this page, since equivalent, unaffected exercises (#47, #51) were available.