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Mathematics · Ch 7 — Conic Sections

Focal Properties and Latus Rectum of an Ellipse

7.2.2

Focal Properties and Latus Rectum of an Ellipse

This section collects the key derived facts about the standard ellipse, each following from the defining relations b2=a2(1−e2)b^2=a^2(1-e^2) and the two-focus, two-directrix picture of section 7.2.1.

1. Distance between the directrices. Since the two directrices are x=a/ex=a/e and x=−a/ex=-a/e, the distance between them is simply

d(dd′)=∣ae−(−ae)∣=2ae.d(dd')=\left|\dfrac{a}{e}-\left(-\dfrac{a}{e}\right)\right|=\dfrac{2a}{e}.

2. End points of the latus rectum. Let LSL′LSL' be the latus rectum through the (right) focus S(ae,0)S(ae,0); write L≡(ae,l)L\equiv(ae,l) for the upper end point. Since LL lies on the ellipse:

(ae)2a2+l2b2=1  ⟹  e2+l2b2=1  ⟹  l2=b2(1−e2).\dfrac{(ae)^2}{a^2}+\dfrac{l^2}{b^2}=1 \;\Longrightarrow\; e^2+\dfrac{l^2}{b^2}=1 \;\Longrightarrow\; l^2=b^2(1-e^2).

Since b2=a2(1−e2)b^2=a^2(1-e^2), we have 1−e2=b2/a21-e^2=b^2/a^2, so l2=b2⋅b2a2=b4a2l^2=b^2\cdot\dfrac{b^2}{a^2}=\dfrac{b^4}{a^2}, giving l=b2al=\dfrac{b^2}{a} (taking the positive value, first quadrant). So L≡(ae,b2a)L\equiv\left(ae,\dfrac{b^2}{a}\right) and L′≡(ae,−b2a)L'\equiv\left(ae,-\dfrac{b^2}{a}\right).

3. Length of the latus rectum. By symmetry, l(LSL′)=l(SL)+l(SL′)=b2a+b2a=2b2al(LSL')=l(SL)+l(SL')=\dfrac{b^2}{a}+\dfrac{b^2}{a}=\dfrac{2b^2}{a}.

4. Sum of focal distances is constant — the "pin and string" property. For a point PP on the ellipse, let SPSP and S′PS'P be its distances to the two foci, and PM,PM′PM,PM' its distances to the two directrices. By the focus–directrix property applied to each focus: SP=e⋅PMSP=e\cdot PM and S′P=e⋅PM′S'P=e\cdot PM'. Adding:

SP+S′P=e(PM+PM′)=e⋅(MM′)=e⋅(distance between directrices)=e(2ae)=2a.SP+S'P = e(PM+PM') = e\cdot(MM') = e\cdot(\text{distance between directrices}) = e\left(\dfrac{2a}{e}\right)=2a.

So the sum of the focal distances of any point on the ellipse is the constant 2a2a — the length of the major axis. This is precisely the classical "pin-and-string" construction: fix two pins at S1,S2S_1,S_2 with d(S1S2)<Kd(S_1S_2)<K, loop a string of total length K=2aK=2a around them, and trace a pencil kept taut against the string — the resulting curve is an ellipse with foci S1,S2S_1,S_2.

5. Auxiliary circle. The circle drawn with the major axis AA′AA' as its diameter (so centred at the origin, radius aa) is called the auxiliary circle of the ellipse.

6. Parametric form and the eccentric angle. Let P(x,y)P(x,y) be a point on the ellipse, and let QQ be the point on the auxiliary circle directly above/below PP (i.e. PQ⊥PQ\perp major axis, sharing the same xx-coordinate). Writing ∠XOQ=θ\angle XOQ=\theta, the point QQ on the circle of radius aa is Q=(acos⁡θ, asin⁡θ)Q=(a\cos\theta,\,a\sin\theta), so P=(acos⁡θ, y)P=(a\cos\theta,\,y) for some yy to be found. Substituting into the ellipse equation:

a2cos⁡2θa2+y2b2=1  ⟹  y2b2=1−cos⁡2θ=sin⁡2θ  ⟹  y=±bsin⁡θ.\dfrac{a^2\cos^2\theta}{a^2}+\dfrac{y^2}{b^2}=1 \;\Longrightarrow\; \dfrac{y^2}{b^2}=1-\cos^2\theta=\sin^2\theta \;\Longrightarrow\; y=\pm b\sin\theta.

So P(x,y)≡(acos⁡θ, bsin⁡θ)≡P(θ)P(x,y)\equiv(a\cos\theta,\,b\sin\theta)\equiv P(\theta). This is the parametric form x=acos⁡θ, y=bsin⁡θx=a\cos\theta,\,y=b\sin\theta, and θ\theta is called the eccentric angle of PP (note: θ\theta is generally not the actual angle that OPOP makes with the XX-axis — that would need tan⁡(∠POX)=y/x=(b/a)tan⁡θ\tan(\angle POX)=y/x=(b/a)\tan\theta, a different angle unless a=ba=b). Solving for θ\theta in terms of a given (x,y)(x,y): θ=tan⁡−1(aybx)\theta=\tan^{-1}\left(\dfrac{ay}{bx}\right).

7. The vertical ellipse (b > a). x2a2+y2b2=1\dfrac{x^2}{a^2}+\dfrac{y^2}{b^2}=1 with b>ab>a is the OTHER standard form — here the major axis is along YY instead of XX. Every formula above still applies, but with the roles of a,ba,b and X,YX,Y interchanged (see the comparison table on this section).

Worked Example 1 — full property set for four given ellipses.

  1. x216+y29=1\dfrac{x^2}{16}+\dfrac{y^2}{9}=1: a2=16,b2=9⇒a=4,b=3a^2=16,b^2=9\Rightarrow a=4,b=3; e2=1−916=716⇒e=74e^2=1-\dfrac9{16}=\dfrac7{16}\Rightarrow e=\dfrac{\sqrt7}{4}; foci (±7,0)\left(\pm\sqrt7,0\right); directrices x=±167x=\pm\dfrac{16}{\sqrt7}; latus rectum =2(9)4=92=\dfrac{2(9)}{4}=\dfrac92; parametric form x=4cos⁡θ,y=3sin⁡θx=4\cos\theta,y=3\sin\theta.
  2. 3x2+4y2=13x^2+4y^2=1, i.e. x21/3+y21/4=1\dfrac{x^2}{1/3}+\dfrac{y^2}{1/4}=1: a2=13,b2=14⇒a=13,b=12a^2=\dfrac13,b^2=\dfrac14\Rightarrow a=\dfrac1{\sqrt3},b=\dfrac12 (a>ba>b); e2=1−b2a2=1−34=14⇒e=12e^2=1-\dfrac{b^2}{a^2}=1-\dfrac34=\dfrac14\Rightarrow e=\dfrac12; centre (0,0)(0,0); vertices (±13,0)\left(\pm\dfrac1{\sqrt3},0\right) and (0,±12)\left(0,\pm\dfrac12\right); foci (±123,0)\left(\pm\dfrac1{2\sqrt3},0\right).
  3. 4x2+3y2=14x^2+3y^2=1, i.e. x21/4+y21/3=1\dfrac{x^2}{1/4}+\dfrac{y^2}{1/3}=1: here a2=14,b2=13a^2=\dfrac14,b^2=\dfrac13 with b>ab>a, so the YY-axis is the major axis; e2=1−a2b2=1−34=14⇒e=12e^2=1-\dfrac{a^2}{b^2}=1-\dfrac34=\dfrac14\Rightarrow e=\dfrac12; foci on the YY-axis at (0,±be)(0,\pm be).
  4. 4x2+9y2−16x+54y+61=04x^2+9y^2-16x+54y+61=0: completing the square gives 4(x−2)2+9(y+3)2=364(x-2)^2+9(y+3)^2=36, i.e. (x−2)29+(y+3)24=1\dfrac{(x-2)^2}{9}+\dfrac{(y+3)^2}{4}=1: a2=9,b2=4⇒a=3,b=2a^2=9,b^2=4\Rightarrow a=3,b=2; centre (2,−3)(2,-3); e2=1−49=59⇒e=53e^2=1-\dfrac49=\dfrac59\Rightarrow e=\dfrac{\sqrt5}{3}; vertices at (2±3,−3)=(5,−3),(−1,−3)(2\pm3,-3)=(5,-3),(-1,-3) and (2,−3±2)=(2,−1),(2,−5)(2,-3\pm2)=(2,-1),(2,-5). …
Figure 7.17Sum of focal distances

What this figure shows. A point PP on the ellipse with segments SPSP and S′PS'P drawn to both foci, illustrating SP+S′P=2aSP+S'P=2a. This figure gives the reader a concrete visual reference for the geometric configuration described in the surrounding text, tying the abstract statement to a picture …

Figure 7.18Auxiliary circle and eccentric angle

What this figure shows. The auxiliary circle (radius aa) with a point QQ on it and the corresponding point PP on the ellipse directly below/above QQ, both sharing the same eccentric angle θ\theta. …

Table 2.2-TEllipse properties: $a>b$ vs $b>a$ (vertical) form
Termx2a2+y2b2=1, a>b\frac{x^2}{a^2}+\frac{y^2}{b^2}=1,\ a>bx2a2+y2b2=1, b>a\frac{x^2}{a^2}+\frac{y^2}{b^2}=1,\ b>a
Centre(0,0)(0,0)(0,0)(0,0)
Major / minor axisXX-axis / YY-axisYY-axis / XX-axis
Length of major axis2a2a2b2b
Length of minor axis2b2b2a2a
Relationb2=a2(1−e2)b^2=a^2(1-e^2)a2=b2(1−e2)a^2=b^2(1-e^2)
Foci(±ae,0)(\pm ae,0)(0,±be)(0,\pm be)
Directricesx=±a/ex=\pm a/ey=±b/ey=\pm b/e
Latus rectum length2b2/a2b^2/a2a2/b2a^2/b
Misc 2.2-Ex1Worked Example 1: ellipse properties (four sub-cases)

Worked out. Finds foci, vertices, major-axis length, eccentricity and latus-rectum length for four given ellipses, including two completing-the-square cases. …

Misc 2.2-Ex2Worked Example 2: equation from vertices and foci

Worked out. Finds the standard equation of an ellipse given its vertices (±13,0)(\pm13,0) and foci (±5,0)(\pm5,0). Working through this worked example after reading the theory above helps consolidate the method before attempting the exercise questions that follow it in the textbook. …

Misc 2.2-Ex3Worked Example 3: eccentricity from a latus-rectum ratio

Worked out. Finds the eccentricity of an ellipse whose latus rectum is one third of its minor axis. Working through this worked example after reading the theory above helps consolidate the method before attempting the exercise questions that follow it in the textbook. …

Misc 2.2-ActActivity: equation through two points

Worked out. Sets up (without fully solving) the pair of simultaneous equations for an ellipse with major axis on the X-axis passing through (4,3)(4,3) and (6,2)(6,2). …