Basic Examples on Hyperbolas Set 2

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Example - 4

What is the locus of the center of a circle which touches two given circles of radii \({r_1}\) and \({r_2},\) as shown below, externally ?

Solution : Consider a circle of radius r and center at C, touching both the circles externally, as shown in the figure below :

From the geometry of the figure, it is evident that

\[\begin{align}&\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,C{C_1} = r + {r_1}\\\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,&\qquad\qquad\quad\; C{C_2} = r + {r_2}\\ &\Rightarrow \left| {C{C_1} - C{C_2}} \right| = \left| {{r_1} - {r_2}} \right|\end{align}\]

This relation tells that the center C will always move in such a way so that the difference of its distances from two fixed points (the two centers C1 and C2) is always constant. Thus, the locus of the center C is a hyperbola with the two foci at C1 and C2.

The equation for the locus of C can easily be evaluated by first assuming a coordinate system with the origin at the mid-point of C1C2 and the x-axis along C1C2. Using standard symbols, we have

\[\begin{align}&\qquad\;2a = \left| {{r_1} - {r_2}} \right|\\&\qquad 2ae = d\\& \Rightarrow \quad e = \frac{d}{{\left| {{r_1} - {r_2}} \right|}}\end{align}\]

Since a and e are known, the equation for the hyperbola can now be written.

Example - 5

The equations of the transverse and conjugate axes of a hyperbola are \({L_1}:x + 2y - 3 = 0\) and \({L_2}:2x - y + 4 = 0\) respectively, and their respective lengths are \(\sqrt 2 \) and \(\begin{align}\frac{2}{{\sqrt 3 }}.\end{align}\) What is the equation of the hyperbola ?

Solution: We have,

\[\begin{align}&2a = \sqrt 2 \quad \Rightarrow \quad a = \frac{1}{{\sqrt 2 }}\\&2b = \frac{2}{{\sqrt 3 }} \quad \Rightarrow \quad b = \frac{1}{{\sqrt 3 }}\end{align}\]

We first find out the equation of the hyperbola in the \({L_1} - {L_2}\) system ( in which the coordinates of any point can be represented by \((X,\,\,Y)\). This equation is simply

\[\begin{align}&\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\frac{{{X^2}}}{{{a^2}}} - \frac{{{Y^2}}}{{{b^2}}} = 1\\\\ &\Rightarrow \quad 2{X^2} - 3{Y^2} = 1\qquad\qquad\qquad\qquad  ...\left( 1 \right)\end{align}\]

Now, what do X and Y represent? As we’ve already discussed in the previous chapter X and Y represent the perpendicular distances of the point P(X, Y) from \({L_2}\) and \({L_1}\) respectively

Thus, if in the original x - y system, P has the coordinates (x, y), we have,

\[X = \frac{{\left| {2x - y + 4} \right|}}{{\sqrt 5 }};\,\,\,\,\,Y = \frac{{\left| {x + 2y - 3} \right|}}{{\sqrt 5 }}\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,...\left( 2 \right)\]

Using (2) in (1), the equation of the hyperbola is

\[\frac{2}{5}{(2x - y + 4)^2} - \frac{3}{5}{(x + 2y - 3)^2} = 1\]

which simplifies to

\[{x^2} - 4xy - 2{y^2} + 10x + 4y = 0\]

Example - 6

For a variable parameter t, prove that the locus of the intersection point of the straight lines \(\begin{align}\frac{x}{a} - \frac{y}{b} = t\end{align}\) and \(\begin{align}\frac{x}{a} + \frac{y}{b} = \frac{1}{t}\end{align}\) is a hyperbola.

Solution: Let the point of intersection of the two lines be (h, k).

We have,

\[\begin{align}&\frac{h}{a} - \frac{k}{b} = t\\\\&\frac{h}{a} + \frac{k}{b} = \frac{1}{t}\end{align}\]

Multiplying the two relations (so that t gets eliminated), we obtain

\[\frac{{{h^2}}}{{{a^2}}} - \frac{{{k^2}}}{{{b^2}}} = 1\]

Thus, the locus of the intersection point is

\[\frac{{{x^2}}}{{{a^2}}} - \frac{{{y^2}}}{{{b^2}}} = 1\]

which is a hyperbola.

We will now consider how to represent a hyperbola in parametric form.

Consider the hyperbola \(\begin{align}\frac{{{x^2}}}{{{a^2}}} - \frac{{{y^2}}}{{{b^2}}} = 1.\end{align}\)On the transverse axis AA' as diameter, describe a circle. This circle will obviously touch both the segments of the hyperbola, as shown below. This circle is termed the auxiliary circle of the hyperbola:

Let \(P(x,\,\,y)\) be any point on the hyperbola. Drop a perpendicular PQ from P onto the transverse axis (the x-axis). From Q, draw the tangent QR to the auxiliary circle. In \(\Delta OQR,\)we have

\[\begin{align}&\;\;\;\;\,\,\,\,\,\,\,\,\,\frac{{OR}}{{OQ}} = \cos \theta \\ &\Rightarrow \quad  OQ = OR\sec \theta = a\sec \theta \\ &\Rightarrow \quad x = a\sec \theta\end{align}\]

Thus, the x-coordinate of P in terms of \(\theta \) is \(a  \sec \theta .\) Substituting \(x = a\sec \theta \) in the equation of the hyperbola, we obtain \(y = b\tan \theta .\) Therefore, we can conclude that any point \(\begin{align}P(x,\,\,y)\end {align}\) on the hyperbola \(\begin{align}\frac{{{x^2}}}{{{a^2}}} - \frac{{{y^2}}}{{{b^2}}} = 1\end{align}\) has the equivalent representation \(P(a\sec \theta ,\,b\tan \theta )\):

\[\boxed{P \equiv (x,\,y) \equiv (a\sec \theta ,\,\tan \theta )}\]

This form is know as the parametric form of any point on the hyperbola, the parameter being  \(\theta \)  where \(0 \le \theta < 2\pi .\) The point \((a\sec \theta ,\,\,b\tan \theta )\) is sometimes simply referred to as the point \(\theta .\) (As in ellipses, \(\theta \)  is called the eccentric angle).

From Fig - 10, note that 

\[\frac{{PQ}}{{QR}} = \frac{{b\tan \theta }}{{a\tan \theta }} = \frac{b}{a} = {\rm{constant}}\]

Thus, for any point P on the hyperbola, the ratio \(\begin{align}\frac{{PQ}}{{QR}}\end{align}\) is always fixed (where PQ and QR have been constructed as described above). In fact, the constancy of this ratio can itself be used to define a hyperbola (starting with the circle \({x^2} + {y^2} = {a^2},\) we draw any tangent to it at a point R to intersect one of the circle’s diameter at Q. From Q, we construct a perpendicular PQ to this diameter, such that \(PQ:QR = \lambda \) which is fixed. As R varies on the circle, P traces out hyperbola.

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