Calculus Volume 2

# 7.5Conic Sections

Calculus Volume 27.5 Conic Sections

### Learning Objectives

• 7.5.1 Identify the equation of a parabola in standard form with given focus and directrix.
• 7.5.2 Identify the equation of an ellipse in standard form with given foci.
• 7.5.3 Identify the equation of a hyperbola in standard form with given foci.
• 7.5.4 Recognize a parabola, ellipse, or hyperbola from its eccentricity value.
• 7.5.5 Write the polar equation of a conic section with eccentricity $ee$.
• 7.5.6 Identify when a general equation of degree two is a parabola, ellipse, or hyperbola.

Conic sections have been studied since the time of the ancient Greeks, and were considered to be an important mathematical concept. As early as 320 BCE, such Greek mathematicians as Menaechmus, Appollonius, and Archimedes were fascinated by these curves. Appollonius wrote an entire eight-volume treatise on conic sections in which he was, for example, able to derive a specific method for identifying a conic section through the use of geometry. Since then, important applications of conic sections have arisen (for example, in astronomy), and the properties of conic sections are used in radio telescopes, satellite dish receivers, and even architecture. In this section we discuss the three basic conic sections, some of their properties, and their equations.

Conic sections get their name because they can be generated by intersecting a plane with a cone. A cone has two identically shaped parts called nappes. One nappe is what most people mean by “cone,” having the shape of a party hat. A right circular cone can be generated by revolving a line passing through the origin around the y-axis as shown.

Figure 7.43 A cone generated by revolving the line $y=3xy=3x$ around the $yy$-axis.

Conic sections are generated by the intersection of a plane with a cone (Figure 7.44). If the plane is parallel to the axis of revolution (the y-axis), then the conic section is a hyperbola. If the plane is parallel to the generating line, the conic section is a parabola. If the plane is perpendicular to the axis of revolution, the conic section is a circle. If the plane intersects one nappe at an angle to the axis (other than $90°),90°),$ then the conic section is an ellipse.

Figure 7.44 The four conic sections. Each conic is determined by the angle the plane makes with the axis of the cone.

### Parabolas

A parabola is generated when a plane intersects a cone parallel to the generating line. In this case, the plane intersects only one of the nappes. A parabola can also be defined in terms of distances.

### Definition

A parabola is the set of all points whose distance from a fixed point, called the focus, is equal to the distance from a fixed line, called the directrix. The point halfway between the focus and the directrix is called the vertex of the parabola.

A graph of a typical parabola appears in Figure 7.45. Using this diagram in conjunction with the distance formula, we can derive an equation for a parabola. Recall the distance formula: Given point P with coordinates $(x1,y1)(x1,y1)$ and point Q with coordinates $(x2,y2),(x2,y2),$ the distance between them is given by the formula

$d(P,Q)=(x2−x1)2+(y2−y1)2.d(P,Q)=(x2−x1)2+(y2−y1)2.$

Then from the definition of a parabola and Figure 7.45, we get

$d(F,P)=d(P,Q)(0−x)2+(p−y)2=(x−x)2+(−p−y)2.d(F,P)=d(P,Q)(0−x)2+(p−y)2=(x−x)2+(−p−y)2.$

Squaring both sides and simplifying yields

$x2+(p−y)2=02+(−p−y)2x2+p2−2py+y2=p2+2py+y2x2−2py=2pyx2=4py.x2+(p−y)2=02+(−p−y)2x2+p2−2py+y2=p2+2py+y2x2−2py=2pyx2=4py.$
Figure 7.45 A typical parabola in which the distance from the focus to the vertex is represented by the variable $p.p.$

Now suppose we want to relocate the vertex. We use the variables $(h,k)(h,k)$ to denote the coordinates of the vertex. Then if the focus is directly above the vertex, it has coordinates $(h,k+p)(h,k+p)$ and the directrix has the equation $y=k−p.y=k−p.$ Going through the same derivation yields the formula $(x−h)2=4p(y−k).(x−h)2=4p(y−k).$ Solving this equation for y leads to the following theorem.

Theorem 7.8

#### Equations for Parabolas

Given a parabola opening upward with vertex located at $(h,k)(h,k)$ and focus located at $(h,k+p),(h,k+p),$ where p is a constant, the equation for the parabola is given by

$y=14p(x−h)2+k.y=14p(x−h)2+k.$
7.11

This is the standard form of a parabola.

We can also study the cases when the parabola opens down or to the left or the right. The equation for each of these cases can also be written in standard form as shown in the following graphs.

Figure 7.46 Four parabolas, opening in various directions, along with their equations in standard form.

In addition, the equation of a parabola can be written in the general form, though in this form the values of h, k, and p are not immediately recognizable. The general form of a parabola is written as

$ax2+bx+cy+d=0oray2+bx+cy+d=0.ax2+bx+cy+d=0oray2+bx+cy+d=0.$

The first equation represents a parabola that opens either up or down. The second equation represents a parabola that opens either to the left or to the right. To put the equation into standard form, use the method of completing the square.

### Example 7.19

#### Converting the Equation of a Parabola from General into Standard Form

Put the equation $x2−4x−8y+12=0x2−4x−8y+12=0$ into standard form and graph the resulting parabola.

Checkpoint 7.18

Put the equation $2y2−x+12y+16=02y2−x+12y+16=0$ into standard form and graph the resulting parabola.

The axis of symmetry of a vertical (opening up or down) parabola is a vertical line passing through the vertex. The parabola has an interesting reflective property. Suppose we have a satellite dish with a parabolic cross section. If a beam of electromagnetic waves, such as light or radio waves, comes into the dish in a straight line from a satellite (parallel to the axis of symmetry), then the waves reflect off the dish and collect at the focus of the parabola as shown. Consider a parabolic dish designed to collect signals from a satellite in space. The dish is aimed directly at the satellite, and a receiver is located at the focus of the parabola. Radio waves coming in from the satellite are reflected off the surface of the parabola to the receiver, which collects and decodes the digital signals. This allows a small receiver to gather signals from a wide angle of sky. Flashlights and headlights in a car work on the same principle, but in reverse: the source of the light (that is, the light bulb) is located at the focus and the reflecting surface on the parabolic mirror focuses the beam straight ahead. This allows a small light bulb to illuminate a wide angle of space in front of the flashlight or car.

### Ellipses

An ellipse can also be defined in terms of distances. In the case of an ellipse, there are two foci (plural of focus), and two directrices (plural of directrix). We look at the directrices in more detail later in this section.

### Definition

An ellipse is the set of all points for which the sum of their distances from two fixed points (the foci) is constant.

Figure 7.48 A typical ellipse in which the sum of the distances from any point on the ellipse to the foci is constant.

A graph of a typical ellipse is shown in Figure 7.48. In this figure the foci are labeled as $FF$ and $F′.F′.$ Both are the same fixed distance from the origin, and this distance is represented by the variable c. Therefore the coordinates of $FF$ are $(c,0)(c,0)$ and the coordinates of $F′F′$ are $(−c,0).(−c,0).$ The points $PP$ and $P′P′$ are located at the ends of the major axis of the ellipse, and have coordinates $(a,0)(a,0)$ and $(−a,0),(−a,0),$ respectively. The major axis is always the longest distance across the ellipse, and can be horizontal or vertical. Thus, the length of the major axis in this ellipse is 2a. Furthermore, $PP$ and $P′P′$ are called the vertices of the ellipse. The points $QQ$ and $Q′Q′$ are located at the ends of the minor axis of the ellipse, and have coordinates $(0,b)(0,b)$ and $(0,−b),(0,−b),$ respectively. The minor axis is the shortest distance across the ellipse. The minor axis is perpendicular to the major axis.

According to the definition of the ellipse, we can choose any point on the ellipse and the sum of the distances from this point to the two foci is constant. Suppose we choose the point P. Since the coordinates of point P are $(a,0),(a,0),$ the sum of the distances is

$d(P,F)+d(P,F′)=(a−c)+(a+c)=2a.d(P,F)+d(P,F′)=(a−c)+(a+c)=2a.$

Therefore the sum of the distances from an arbitrary point A with coordinates $(x,y)(x,y)$ is also equal to 2a. Using the distance formula, we get

$d(A,F)+d(A,F′)=2a(x−c)2+y2+(x+c)2+y2=2a.d(A,F)+d(A,F′)=2a(x−c)2+y2+(x+c)2+y2=2a.$

Subtract the second radical from both sides and square both sides:

$(x−c)2+y2=2a−(x+c)2+y2(x−c)2+y2=4a2−4a(x+c)2+y2+(x+c)2+y2x2−2cx+c2+y2=4a2−4a(x+c)2+y2+x2+2cx+c2+y2−2cx=4a2−4a(x+c)2+y2+2cx.(x−c)2+y2=2a−(x+c)2+y2(x−c)2+y2=4a2−4a(x+c)2+y2+(x+c)2+y2x2−2cx+c2+y2=4a2−4a(x+c)2+y2+x2+2cx+c2+y2−2cx=4a2−4a(x+c)2+y2+2cx.$

Now isolate the radical on the right-hand side and square again:

$−2cx=4a2−4a(x+c)2+y2+2cx4a(x+c)2+y2=4a2+4cx(x+c)2+y2=a+cxa(x+c)2+y2=a2+2cx+c2x2a2x2+2cx+c2+y2=a2+2cx+c2x2a2x2+c2+y2=a2+c2x2a2.−2cx=4a2−4a(x+c)2+y2+2cx4a(x+c)2+y2=4a2+4cx(x+c)2+y2=a+cxa(x+c)2+y2=a2+2cx+c2x2a2x2+2cx+c2+y2=a2+2cx+c2x2a2x2+c2+y2=a2+c2x2a2.$

Isolate the variables on the left-hand side of the equation and the constants on the right-hand side:

$x2−c2x2a2+y2=a2−c2(a2−c2)x2a2+y2=a2−c2.x2−c2x2a2+y2=a2−c2(a2−c2)x2a2+y2=a2−c2.$

Divide both sides by $a2−c2.a2−c2.$ This gives the equation

$x2a2+y2a2−c2=1.x2a2+y2a2−c2=1.$

If we refer back to Figure 7.48, then the length of each of the two green line segments is equal to a. This is true because the sum of the distances from the point Q to the foci $FandF′FandF′$ is equal to 2a, and the lengths of these two line segments are equal. This line segment forms a right triangle with hypotenuse length a and leg lengths b and c. From the Pythagorean theorem, $a2=b2=c2a2=b2=c2$ and $b2+a2−c2.b2+a2−c2.$ Therefore the equation of the ellipse becomes

$x2a2+y2b2=1.x2a2+y2b2=1.$

Finally, if the center of the ellipse is moved from the origin to a point $(h,k),(h,k),$ we have the following standard form of an ellipse.

Theorem 7.9

#### Equation of an Ellipse in Standard Form

Consider the ellipse with center $(h,k),(h,k),$ a horizontal major axis with length 2a, and a vertical minor axis with length 2b. Then the equation of this ellipse in standard form is

$(x−h)2a2+(y−k)2b2=1(x−h)2a2+(y−k)2b2=1$
7.12

and the foci are located at $(h±c,k),(h±c,k),$ where $c2=a2−b2.c2=a2−b2.$ The equations of the directrices are $x=h±a2c.x=h±a2c.$

If the major axis is vertical, then the equation of the ellipse becomes

$(x−h)2b2+(y−k)2a2=1(x−h)2b2+(y−k)2a2=1$
7.13

and the foci are located at $(h,k±c),(h,k±c),$ where $c2=a2−b2.c2=a2−b2.$ The equations of the directrices in this case are $y=k±a2c.y=k±a2c.$

If the major axis is horizontal, then the ellipse is called horizontal, and if the major axis is vertical, then the ellipse is called vertical. The equation of an ellipse is in general form if it is in the form $Ax2+By2+Cx+Dy+E=0,Ax2+By2+Cx+Dy+E=0,$ where A and B are either both positive or both negative. To convert the equation from general to standard form, use the method of completing the square.

### Example 7.20

#### Finding the Standard Form of an Ellipse

Put the equation $9x2+4y2−36x+24y+36=09x2+4y2−36x+24y+36=0$ into standard form and graph the resulting ellipse.

Checkpoint 7.19

Put the equation $9x2+16y2+18x−64y−71=09x2+16y2+18x−64y−71=0$ into standard form and graph the resulting ellipse.

According to Kepler’s first law of planetary motion, the orbit of a planet around the Sun is an ellipse with the Sun at one of the foci as shown in Figure 7.50(a). Because Earth’s orbit is an ellipse, the distance from the Sun varies throughout the year. A commonly held misconception is that Earth is closer to the Sun in the summer. In fact, in summer for the northern hemisphere, Earth is farther from the Sun than during winter. The difference in season is caused by the tilt of Earth’s axis in the orbital plane. Comets that orbit the Sun, such as Halley’s Comet, also have elliptical orbits, as do moons orbiting the planets and satellites orbiting Earth.

Ellipses also have interesting reflective properties: A light ray emanating from one focus passes through the other focus after mirror reflection in the ellipse. The same thing occurs with a sound wave as well. The National Statuary Hall in the U.S. Capitol in Washington, DC, is a famous room in an elliptical shape as shown in Figure 7.50(b). This hall served as the meeting place for the U.S. House of Representatives for almost fifty years. The location of the two foci of this semi-elliptical room are clearly identified by marks on the floor, and even if the room is full of visitors, when two people stand on these spots and speak to each other, they can hear each other much more clearly than they can hear someone standing close by. Legend has it that John Quincy Adams had his desk located on one of the foci and was able to eavesdrop on everyone else in the House without ever needing to stand. Although this makes a good story, it is unlikely to be true, because the original ceiling produced so many echoes that the entire room had to be hung with carpets to dampen the noise. The ceiling was rebuilt in 1902 and only then did the now-famous whispering effect emerge. Another famous whispering gallery—the site of many marriage proposals—is in Grand Central Station in New York City.

Figure 7.50 (a) Earth’s orbit around the Sun is an ellipse with the Sun at one focus. (b) Statuary Hall in the U.S. Capitol is a whispering gallery with an elliptical cross section.

### Hyperbolas

A hyperbola can also be defined in terms of distances. In the case of a hyperbola, there are two foci and two directrices. Hyperbolas also have two asymptotes.

### Definition

A hyperbola is the set of all points where the difference between their distances from two fixed points (the foci) is constant.

A graph of a typical hyperbola appears as follows.

Figure 7.51 A typical hyperbola in which the difference of the distances from any point on the ellipse to the foci is constant. The transverse axis is also called the major axis, and the conjugate axis is also called the minor axis.

The derivation of the equation of a hyperbola in standard form is virtually identical to that of an ellipse. One slight hitch lies in the definition: The difference between two numbers is always positive. Let P be a point on the hyperbola with coordinates $(x,y).(x,y).$ Then the definition of the hyperbola gives $|d(P,F1)−d(P,F2)|=constant.|d(P,F1)−d(P,F2)|=constant.$ To simplify the derivation, assume that P is on the right branch of the hyperbola, so the absolute value bars drop. If it is on the left branch, then the subtraction is reversed. The vertex of the right branch has coordinates $(a,0),(a,0),$ so

$d(P,F1)−d(P,F2)=(c+a)−(c−a)=2a.d(P,F1)−d(P,F2)=(c+a)−(c−a)=2a.$

This equation is therefore true for any point on the hyperbola. Returning to the coordinates $(x,y)(x,y)$ for P:

$d(P,F1)−d(P,F2)=2a(x+c)2+y2−(x−c)2+y2=2a.d(P,F1)−d(P,F2)=2a(x+c)2+y2−(x−c)2+y2=2a.$

$(x−c)2+y2=2a+(x+c)2+y2(x−c)2+y2=4a2+4a(x+c)2+y2+(x+c)2+y2x2−2cx+c2+y2=4a2+4a(x+c)2+y2+x2+2cx+c2+y2−2cx=4a2+4a(x+c)2+y2+2cx.(x−c)2+y2=2a+(x+c)2+y2(x−c)2+y2=4a2+4a(x+c)2+y2+(x+c)2+y2x2−2cx+c2+y2=4a2+4a(x+c)2+y2+x2+2cx+c2+y2−2cx=4a2+4a(x+c)2+y2+2cx.$

Now isolate the radical on the right-hand side and square again:

$−2cx=4a2+4a(x+c)2+y2+2cx4a(x+c)2+y2=−4a2−4cx(x+c)2+y2=−a−cxa(x+c)2+y2=a2+2cx+c2x2a2x2+2cx+c2+y2=a2+2cx+c2x2a2x2+c2+y2=a2+c2x2a2.−2cx=4a2+4a(x+c)2+y2+2cx4a(x+c)2+y2=−4a2−4cx(x+c)2+y2=−a−cxa(x+c)2+y2=a2+2cx+c2x2a2x2+2cx+c2+y2=a2+2cx+c2x2a2x2+c2+y2=a2+c2x2a2.$

Isolate the variables on the left-hand side of the equation and the constants on the right-hand side:

$x2−c2x2a2+y2=a2−c2(a2−c2)x2a2+y2=a2−c2.x2−c2x2a2+y2=a2−c2(a2−c2)x2a2+y2=a2−c2.$

Finally, divide both sides by $a2−c2.a2−c2.$ This gives the equation

$x2a2+y2a2−c2=1.x2a2+y2a2−c2=1.$

We now define b so that $b2=c2−a2.b2=c2−a2.$ This is possible because $c>a.c>a.$ Therefore the equation of the ellipse becomes

$x2a2−y2b2=1.x2a2−y2b2=1.$

Finally, if the center of the hyperbola is moved from the origin to the point $(h,k),(h,k),$ we have the following standard form of a hyperbola.

Theorem 7.10

#### Equation of a Hyperbola in Standard Form

Consider the hyperbola with center $(h,k),(h,k),$ a horizontal major axis, and a vertical minor axis. Then the equation of this ellipse is

$(x−h)2a2−(y−k)2b2=1(x−h)2a2−(y−k)2b2=1$
7.14

and the foci are located at $(h±c,k),(h±c,k),$ where $c2=a2+b2.c2=a2+b2.$ The equations of the asymptotes are given by $y=k±ba(x−h).y=k±ba(x−h).$ The equations of the directrices are

$x=k±a2a2+b2=h±a2c.x=k±a2a2+b2=h±a2c.$

If the major axis is vertical, then the equation of the hyperbola becomes

$(y−k)2a2−(x−h)2b2=1(y−k)2a2−(x−h)2b2=1$
7.15

and the foci are located at $(h,k±c),(h,k±c),$ where $c2=a2+b2.c2=a2+b2.$ The equations of the asymptotes are given by $y=k±ab(x−h).y=k±ab(x−h).$ The equations of the directrices are

$y=k±a2a2+b2=k±a2c.y=k±a2a2+b2=k±a2c.$

If the major axis (transverse axis) is horizontal, then the hyperbola is called horizontal, and if the major axis is vertical then the hyperbola is called vertical. The equation of a hyperbola is in general form if it is in the form $Ax2+By2+Cx+Dy+E=0,Ax2+By2+Cx+Dy+E=0,$ where A and B have opposite signs. In order to convert the equation from general to standard form, use the method of completing the square.

### Example 7.21

#### Finding the Standard Form of a Hyperbola

Put the equation $9x2−16y2+36x+32y−124=09x2−16y2+36x+32y−124=0$ into standard form and graph the resulting hyperbola. What are the equations of the asymptotes?

Checkpoint 7.20

Put the equation $4y2−9x2+16y+18x−29=04y2−9x2+16y+18x−29=0$ into standard form and graph the resulting hyperbola. What are the equations of the asymptotes?

Hyperbolas also have interesting reflective properties. A ray directed toward one focus of a hyperbola is reflected by a hyperbolic mirror toward the other focus. This concept is illustrated in the following figure.

Figure 7.53 A hyperbolic mirror used to collect light from distant stars.

This property of the hyperbola has important applications. It is used in radio direction finding (since the difference in signals from two towers is constant along hyperbolas), and in the construction of mirrors inside telescopes (to reflect light coming from the parabolic mirror to the eyepiece). Another interesting fact about hyperbolas is that for a comet entering the solar system, if the speed is great enough to escape the Sun’s gravitational pull, then the path that the comet takes as it passes through the solar system is hyperbolic.

### Eccentricity and Directrix

An alternative way to describe a conic section involves the directrices, the foci, and a new property called eccentricity. We will see that the value of the eccentricity of a conic section can uniquely define that conic.

### Definition

The eccentricity e of a conic section is defined to be the distance from any point on the conic section to its focus, divided by the perpendicular distance from that point to the nearest directrix. This value is constant for any conic section, and can define the conic section as well:

1. If $e=1,e=1,$ the conic is a parabola.
2. If $e<1,e<1,$ it is an ellipse.
3. If $e>1,e>1,$ it is a hyperbola.

The eccentricity of a circle is zero. The directrix of a conic section is the line that, together with the point known as the focus, serves to define a conic section. Hyperbolas and noncircular ellipses have two foci and two associated directrices. Parabolas have one focus and one directrix.

The three conic sections with their directrices appear in the following figure.

Figure 7.54 The three conic sections with their foci and directrices.

Recall from the definition of a parabola that the distance from any point on the parabola to the focus is equal to the distance from that same point to the directrix. Therefore, by definition, the eccentricity of a parabola must be 1. The equations of the directrices of a horizontal ellipse are $x=±a2c.x=±a2c.$ The right vertex of the ellipse is located at $(a,0)(a,0)$ and the right focus is $(c,0).(c,0).$ Therefore the distance from the vertex to the focus is $a−ca−c$ and the distance from the vertex to the right directrix is $a2c−c.a2c−c.$ This gives the eccentricity as

$e=a−ca2c−a=c(a−c)a2−ac=c(a−c)a(a−c)=ca.e=a−ca2c−a=c(a−c)a2−ac=c(a−c)a(a−c)=ca.$

Since $c this step proves that the eccentricity of an ellipse is less than 1. The directrices of a horizontal hyperbola are also located at $x=±a2c,x=±a2c,$ and a similar calculation shows that the eccentricity of a hyperbola is also $e=ca.e=ca.$ However in this case we have $c>a,c>a,$ so the eccentricity of a hyperbola is greater than 1.

### Example 7.22

#### Determining Eccentricity of a Conic Section

Determine the eccentricity of the ellipse described by the equation

$(x−3)216+(y+2)225=1.(x−3)216+(y+2)225=1.$
Checkpoint 7.21

Determine the eccentricity of the hyperbola described by the equation

$(y−3)249−(x+2)225=1.(y−3)249−(x+2)225=1.$

### Polar Equations of Conic Sections

Sometimes it is useful to write or identify the equation of a conic section in polar form. To do this, we need the concept of the focal parameter. The focal parameter of a conic section p is defined as the distance from a focus to the nearest directrix. The following table gives the focal parameters for the different types of conics, where a is the length of the semi-major axis (i.e., half the length of the major axis), c is the distance from the origin to the focus, and e is the eccentricity. In the case of a parabola, a represents the distance from the vertex to the focus.

Conic e p
Ellipse $0 $a2−c2c=a(1−e2)ca2−c2c=a(1−e2)c$
Parabola $e=1e=1$ $2a2a$
Hyperbola $e>1e>1$ $c2−a2c=a(e2−1)ec2−a2c=a(e2−1)e$
Table 7.1 Eccentricities and Focal Parameters of the Conic Sections

Using the definitions of the focal parameter and eccentricity of the conic section, we can derive an equation for any conic section in polar coordinates. In particular, we assume that one of the foci of a given conic section lies at the pole. Then using the definition of the various conic sections in terms of distances, it is possible to prove the following theorem.

Theorem 7.11

#### Polar Equation of Conic Sections

The polar equation of a conic section with focal parameter p is given by

$r=ep1±ecosθorr=ep1±esinθ.r=ep1±ecosθorr=ep1±esinθ.$

In the equation on the left, the major axis of the conic section is horizontal, and in the equation on the right, the major axis is vertical. To work with a conic section written in polar form, first make the constant term in the denominator equal to 1. This can be done by dividing both the numerator and the denominator of the fraction by the constant that appears in front of the plus or minus in the denominator. Then the coefficient of the sine or cosine in the denominator is the eccentricity. This value identifies the conic. If cosine appears in the denominator, then the conic is horizontal. If sine appears, then the conic is vertical. If both appear then the axes are rotated. The center of the conic is not necessarily at the origin. The center is at the origin only if the conic is a circle (i.e., $e=0).e=0).$

### Example 7.23

#### Graphing a Conic Section in Polar Coordinates

Identify and create a graph of the conic section described by the equation

$r=31+2cosθ.r=31+2cosθ.$
Checkpoint 7.22

Identify and create a graph of the conic section described by the equation

$r=41−0.8sinθ.r=41−0.8sinθ.$

### General Equations of Degree Two

A general equation of degree two can be written in the form

$Ax2+Bxy+Cy2+Dx+Ey+F=0.Ax2+Bxy+Cy2+Dx+Ey+F=0.$

The graph of an equation of this form is a conic section. If $B≠0B≠0$ then the coordinate axes are rotated. To identify the conic section, we use the discriminant of the conic section $4AC−B2.4AC−B2.$ One of the following cases must be true:

1. $4AC−B2>0.4AC−B2>0.$ If so, the graph is an ellipse.
2. $4AC−B2=0.4AC−B2=0.$ If so, the graph is a parabola.
3. $4AC−B2<0.4AC−B2<0.$ If so, the graph is a hyperbola.

The simplest example of a second-degree equation involving a cross term is $xy=1.xy=1.$ This equation can be solved for y to obtain $y=1x.y=1x.$ The graph of this function is called a rectangular hyperbola as shown.

Figure 7.56 Graph of the equation $xy=1;xy=1;$ The red lines indicate the rotated axes.

The asymptotes of this hyperbola are the x and y coordinate axes. To determine the angle $θθ$ of rotation of the conic section, we use the formula $cot2θ=A−CB.cot2θ=A−CB.$ In this case $A=C=0A=C=0$ and $B=1,B=1,$ so $cot2θ=(0−0)/1=0cot2θ=(0−0)/1=0$ and $θ=45°.θ=45°.$ The method for graphing a conic section with rotated axes involves determining the coefficients of the conic in the rotated coordinate system. The new coefficients are labeled $A′,B′,C′,D′,E′,andF′,A′,B′,C′,D′,E′,andF′,$ and are given by the formulas

$A′=Acos2θ+Bcosθsinθ+Csin2θB′=0C′=Asin2θ−Bsinθcosθ+Ccos2θD′=Dcosθ+EsinθE′=−Dsinθ+EcosθF′=F.A′=Acos2θ+Bcosθsinθ+Csin2θB′=0C′=Asin2θ−Bsinθcosθ+Ccos2θD′=Dcosθ+EsinθE′=−Dsinθ+EcosθF′=F.$

The procedure for graphing a rotated conic is the following:

1. Identify the conic section using the discriminant $4AC−B2.4AC−B2.$
2. Determine $θθ$ using the formula $cot2θ=A−CB.cot2θ=A−CB.$
3. Calculate $A′,B′,C′,D′,E′,andF′.A′,B′,C′,D′,E′,andF′.$
4. Rewrite the original equation using $A′,B′,C′,D′,E′,andF′.A′,B′,C′,D′,E′,andF′.$
5. Draw a graph using the rotated equation.

### Example 7.24

#### Identifying a Rotated Conic

Identify the conic and calculate the angle of rotation of axes for the curve described by the equation

$13x2−63xy+7y2−256=0.13x2−63xy+7y2−256=0.$
Checkpoint 7.23

Identify the conic and calculate the angle of rotation of axes for the curve described by the equation

$3x2+5xy−2y2−125=0.3x2+5xy−2y2−125=0.$

### Section 7.5 Exercises

For the following exercises, determine the equation of the parabola using the information given.

255.

Focus $(4,0)(4,0)$ and directrix $x=−4x=−4$

256.

Focus $(0,−3)(0,−3)$ and directrix $y=3y=3$

257.

Focus $(0,0.5)(0,0.5)$ and directrix $y=−0.5y=−0.5$

258.

Focus $(2,3)(2,3)$ and directrix $x=−2x=−2$

259.

Focus $(0,2)(0,2)$ and directrix $y=4y=4$

260.

Focus $(−1,4)(−1,4)$ and directrix $x=5x=5$

261.

Focus $(−3,5)(−3,5)$ and directrix $y=1y=1$

262.

Focus $(52,−4)(52,−4)$ and directrix $x=72x=72$

For the following exercises, determine the equation of the ellipse using the information given.

263.

Endpoints of major axis at $(4,0),(−4,0)(4,0),(−4,0)$ and foci located at $(2,0),(−2,0)(2,0),(−2,0)$

264.

Endpoints of major axis at $(0,5),(0,−5)(0,5),(0,−5)$ and foci located at $(0,3),(0,−3)(0,3),(0,−3)$

265.

Endpoints of minor axis at $(0,2),(0,−2)(0,2),(0,−2)$ and foci located at $(3,0),(−3,0)(3,0),(−3,0)$

266.

Endpoints of major axis at $(−3,3),(7,3)(−3,3),(7,3)$ and foci located at $(−2,3),(6,3)(−2,3),(6,3)$

267.

Endpoints of major axis at $(−3,5),(−3,−3)(−3,5),(−3,−3)$ and foci located at $(−3,3),(−3,−1)(−3,3),(−3,−1)$

268.

Endpoints of major axis at $(0,0),(0,4)(0,0),(0,4)$ and foci located at $(5,2),(−5,2)(5,2),(−5,2)$

269.

Foci located at $(2,0),(−2,0)(2,0),(−2,0)$ and eccentricity of $1212$

270.

Foci located at $(0,−3),(0,3)(0,−3),(0,3)$ and eccentricity of $3434$

For the following exercises, determine the equation of the hyperbola using the information given.

271.

Vertices located at $(5,0),(−5,0)(5,0),(−5,0)$ and foci located at $(6,0),(−6,0)(6,0),(−6,0)$

272.

Vertices located at $(0,2),(0,−2)(0,2),(0,−2)$ and foci located at $(0,3),(0,−3)(0,3),(0,−3)$

273.

Endpoints of the conjugate axis located at $(0,3),(0,−3)(0,3),(0,−3)$ and foci located $(4,0),(−4,0)(4,0),(−4,0)$

274.

Vertices located at $(0,1),(6,1)(0,1),(6,1)$ and focus located at $(8,1)(8,1)$

275.

Vertices located at $(−2,0),(−2,−4)(−2,0),(−2,−4)$ and focus located at $(−2,−8)(−2,−8)$

276.

Endpoints of the conjugate axis located at $(3,2),(3,4)(3,2),(3,4)$ and focus located at $(3,7)(3,7)$

277.

Foci located at $(6,−0),(6,0)(6,−0),(6,0)$ and eccentricity of 3

278.

$(0,10),(0,−10)(0,10),(0,−10)$ and eccentricity of 2.5

For the following exercises, consider the following polar equations of conics. Determine the eccentricity and identify the conic.

279.

$r=−11+cosθr=−11+cosθ$

280.

$r=82−sinθr=82−sinθ$

281.

$r=52+sinθr=52+sinθ$

282.

$r=5−1+2sinθr=5−1+2sinθ$

283.

$r=32−6sinθr=32−6sinθ$

284.

$r=3−4+3sinθr=3−4+3sinθ$

For the following exercises, find a polar equation of the conic with focus at the origin and eccentricity and directrix as given.

285.

$Directrix:x=4;e=15Directrix:x=4;e=15$

286.

$Directrix:x=−4;e=5Directrix:x=−4;e=5$

287.

$Directrix: y=2;e=2Directrix: y=2;e=2$

288.

$Directrix: y=−2;e=12Directrix: y=−2;e=12$

For the following exercises, sketch the graph of each conic.

289.

$r=11+sinθr=11+sinθ$

290.

$r=11−cosθr=11−cosθ$

291.

$r=41+cosθr=41+cosθ$

292.

$r=105+4sinθr=105+4sinθ$

293.

$r=153−2cosθr=153−2cosθ$

294.

$r=323+5sinθr=323+5sinθ$

295.

$r(2+sinθ)=4r(2+sinθ)=4$

296.

$r=32+6sinθr=32+6sinθ$

297.

$r=3−4+2sinθr=3−4+2sinθ$

298.

$x29+y24=1x29+y24=1$

299.

$x24+y216=1x24+y216=1$

300.

$4x2+9y2=364x2+9y2=36$

301.

$25x2−4y2=10025x2−4y2=100$

302.

$x216−y29=1x216−y29=1$

303.

$x2=12yx2=12y$

304.

$y2=20xy2=20x$

305.

$12x=5y212x=5y2$

For the following equations, determine which of the conic sections is described.

306.

$xy=4xy=4$

307.

$x2+4xy−2y2−6=0x2+4xy−2y2−6=0$

308.

$x2+23xy+3y2−6=0x2+23xy+3y2−6=0$

309.

$x2−xy+y2−2=0x2−xy+y2−2=0$

310.

$34x2−24xy+41y2−25=034x2−24xy+41y2−25=0$

311.

$52x2−72xy+73y2+40x+30y−75=052x2−72xy+73y2+40x+30y−75=0$

312.

The mirror in an automobile headlight has a parabolic cross section, with the lightbulb at the focus. On a schematic, the equation of the parabola is given as $x2=4y.x2=4y.$ At what coordinates should you place the lightbulb?

313.

A satellite dish is shaped like a paraboloid of revolution. The receiver is to be located at the focus. If the dish is 12 feet across at its opening and 4 feet deep at its center, where should the receiver be placed?

314.

Consider the satellite dish of the preceding problem. If the dish is 8 feet across at the opening and 2 feet deep, where should we place the receiver?

315.

A searchlight is shaped like a paraboloid of revolution. A light source is located 1 foot from the base along the axis of symmetry. If the opening of the searchlight is 3 feet across, find the depth.

316.

Whispering galleries are rooms designed with elliptical ceilings. A person standing at one focus can whisper and be heard by a person standing at the other focus because all the sound waves that reach the ceiling are reflected to the other person. If a whispering gallery has a length of 120 feet and the foci are located 30 feet from the center, find the height of the ceiling at the center.

317.

A person is standing 8 feet from the nearest wall in a whispering gallery. If that person is at one focus and the other focus is 80 feet away, what is the length and the height at the center of the gallery?

For the following exercises, determine the polar equation form of the orbit given the length of the major axis and eccentricity for the orbits of the comets or planets. Distance is given in astronomical units (AU).

318.

Halley’s Comet: length of major axis = 35.88, eccentricity = 0.967

319.

Hale-Bopp Comet: length of major axis = 525.91, eccentricity = 0.995

320.

Mars: length of major axis = 3.049, eccentricity = 0.0934

321.

Jupiter: length of major axis = 10.408, eccentricity = 0.0484