Chord of Contact: Definition, Theorem, Equation, Formula

Chord of Contact: Definition, Theorem, Equation, Formula

Komal MiglaniUpdated on 02 Jul 2025, 07:39 PM IST

The concept of a chord bisected at a given point helps in deriving important properties and equations related to circles. Specifically, the equation of such a chord allows for determining its precise location and length, given its midpoint and the circle’s equation. Understanding how to derive and utilize the equation of a chord bisected at a given point is essential for solving complex geometric problems involving circles. It forms the basis for various applications, from calculating the length of a chord to analyzing its position relative to the centre of the circle.

Chord of Contact: Definition, Theorem, Equation, Formula
Chord of Contact: Definition, Theorem, Equation, Formula

Equation of Chord Bisected at a Given Point

A circle is the locus of a moving point such that its distance from a fixed point is constant.

The fixed point is called the centre (O) of the circle and the constant distance is called its radius (r)

A chord of a circle is a line segment with both endpoints on the circle. An interesting geometric property of chords is that they can be uniquely defined by their midpoint when they are bisected at that point.

The equation of the chord (AB) of the circle S = 0 whose midpoint is M(x1,y1) is

$\mathrm{xx}_1+\mathrm{yy}_1-\mathbf{a}^2=\mathrm{x}_1^2+\mathbf{y}_1^2-\mathbf{a}^2 \quad$ or $\quad \mathbf{T}=\mathbf{S}_1$

coordinate of point O is $(0,0)$ and Point M is $\left(x_1, y_1\right)$
slope of $O M=\frac{0-y_1}{0-\mathrm{x}_1}=\frac{\mathrm{y}_1}{\mathrm{x}_1}$
$\therefore$ slope of $\mathrm{AB}=-\frac{\mathrm{x}_1}{\mathrm{y}_1}$
the, equation of $A B$ is $y-y_1=-\frac{x_1}{y_1}\left(x-x_1\right)$
or

$\mathrm{yy}_1-\mathrm{y}_1^2=\mathrm{xx}_1+\mathrm{x}_1^2$

or

$\mathrm{xx}_1+\mathrm{yy}_1-\mathrm{a}^2=\mathrm{x}_1^2+\mathrm{y}_1^2-\mathrm{a}^2 \quad \text { or } \quad \mathbf{T}=\mathbf{S}_1$

Note:

Same result $T=S_1$ can also be applied to get a chord bisected at a given point for any circle of type

$x^2+y^2+2 g x+2 f y+c=0$ as well. as well.

Recommended Video Based on Equation of Chord Bisected at a Given Point


Solved Examples Based on Equation of Chord Bisected at a Given Point

Example 1: Let the tangents at two points A and B on the circle $\mathrm{x}^2+\mathrm{y}^2-4 \mathrm{x}+3=0$ meet at origin $\mathrm{O}(0,0)$. Then the area of the triangle OAB is:
1) $\frac{3 \sqrt{3}}{2}$
2) $\frac{3 \sqrt{3}}{4}$
3) $\frac{3}{2 \sqrt{3}}$
4) $\frac{3}{4 \sqrt{3}}$

Solution

$\begin{aligned}
& \mathrm{r}=\sqrt{4-3}=1 \\
& \mathrm{OA}=\sqrt{\mathrm{s}_1}=\sqrt{3} \\
& \therefore \tan \theta=\frac{1}{\sqrt{3}}
\end{aligned}$

$\begin{aligned}
& \text { Area of } \mathrm{OAB}=2 \times\left(\frac{1}{2} \times \sqrt{3} \cos \theta \cdot \sqrt{3} \sin \theta\right) \\
& =3 \sin \theta \cdot \cos \theta \\
& =3 \times \frac{1}{2} \times \frac{\sqrt{3}}{2} \\
& =\frac{3 \sqrt{3}}{4}
\end{aligned}$

$\therefore$ Option (B)

Example 2: Let AB be a chord of length 12 of the circle $(x-2)^2+(y+1)^2=\frac{169}{4}$. If tangents drawn to the circle at points A and B intersect at the point P , then five times the distance of point P from chord AB is equal to

1) 72

2) 30

3) 34

4) 65

Solution

$\begin{aligned}
& \sin \theta=\frac{\mathrm{BE}}{\mathrm{BC}}=\frac{6}{\frac{13}{2}}=\frac{12}{13} \\
& \text { Now } \frac{\mathrm{BE}}{\rho \mathrm{E}}=\tan (90-\theta) \\
& \Rightarrow \frac{6}{\mathrm{PE}}=\cot \theta \\
& \Rightarrow \mathrm{PE}=6 \tan \theta=6 \cdot \frac{12}{5}=\frac{72}{5} \\
& \Rightarrow 5 \mathrm{PE}=72 \\
& \text { Ans }: 72
\end{aligned}
$
Example 3: Let B be the centre of the circle $x^2+y^2-2 x+4 y+1=0$. Let the tangents at two points P and Q on the circle intersect at the point $\mathrm{A}(3,1)$. Then $\left.8 \cdot\left(\frac{\text { area }}{\text { area } \triangle \mathrm{APQ}}\right) \mathrm{BPQ}\right)$ is equal to $\qquad$

1) 18

2) 34

3) 6

4) 7

Solution

$B=(1,-2), r=\sqrt{1+4-1}=2$

$
\begin{aligned}
& \triangle A P Q=\frac{1}{2} L^2 \sin \theta \text { where L=length of tangent } \\
& =\sqrt{S_1} \\
& =\sqrt{9+1-6+4+1} \\
& =3 \\
& \Rightarrow \triangle A P Q=\frac{1}{2} \times 9 \sin \theta \\
& \triangle B P Q=\frac{1}{2} R^2 \sin (\pi-\theta)=\frac{1}{2} \times 4 \sin \theta \\
& 8 \times \frac{\Delta A P Q}{\Delta B P Q}=8 \times \frac{9}{4}=18
\end{aligned}
$

Example 4: The equation of the chord of contact of the origin w.r.t. circle $x^2+y^2-2 x-4 y-4=0$ is
1) $x+2 y+4=0$
2) $x+2 y-4=0$
3) no chord of contact exist
4) none of these

Solution
Fince $S(0,0)=-4<0$
$\therefore \quad(0,0)$ is inside the circle. So no chord of contact exists.
Hence, the answer is the option (3).

Example 5: Equation of chord AB of circle $\mathrm{x}^2+\mathrm{y}^2=2$ passing through $\mathrm{P}(2,2)$ such that $\mathrm{PB} / \mathrm{PA}=3$, is given by:
1) $x=3 y$
2) $x=y$
3) $y-2=\sqrt{3}(x-2)$
4) none of these

Solution
Key concept: Using the concept of the parametric equation of any line. PB and PA. Let the roots be $\mathrm{r}_1$ and $\mathrm{r}_2$.
Then $\frac{\mathrm{PB}}{\mathrm{PA}}=\frac{\mathrm{r}_2}{\mathrm{r}_1}$, now if $\mathrm{r}_1=\alpha, \mathrm{r}_2=3 \alpha$.
then $4 \alpha=-4(\sin \theta+\cos \theta), 3 \alpha^2=6 \Rightarrow \sin 2 \theta=1 \Rightarrow \theta=\pi / 4$
So, the required chord will be $\mathrm{y}-2=1(\mathrm{x}-2) \Rightarrow \mathrm{y}=\mathrm{x}$

Alternative solution:
Key concept: Using the basic property of a circle.

$
\mathrm{PA} \cdot \mathrm{PB}=\mathrm{PT}^2=2^2+2^2-2=6
$
$
\frac{\mathrm{PB}}{\mathrm{PA}}=3
$

From (1) and (2), we have

$
\mathrm{PA}=\sqrt{2}, \mathrm{~PB}=3 \sqrt{2}
$

$\Rightarrow \mathrm{AB}=2 \sqrt{2}$. Now the diameter of the circle is $2 \sqrt{2}$ (as the radius is $\sqrt{2}$ )
Hence line passes through the centre

$
\Rightarrow \mathrm{y}=\mathrm{x}
$

Hence, the answer is the option (2)

Frequently Asked Questions (FAQs)

Q: What's the significance of the chord of contact in the study of pencils of tangents to a conic section?
A:
The chord of contact is crucial in studying pencils of tangents to a conic
Q: How can the chord of contact be used to study the properties of conjugate diameters in ellipses and hyperbolas?
A:
The chord of contact can be used to identify conjugate diameters in ellipses and hyperbolas. If the chord of contact for an external point is parallel to a diameter, then the line joining the center to the external point is conjugate to that diameter. This relationship helps in understanding the properties of conjugate diameters and their applications in conic sections.
Q: How does the chord of contact theorem help in understanding the properties of focal chords in conic sections?
A:
The chord of contact theorem can be applied to focal chords (chords passing through a focus) to derive important properties. For instance, in an ellipse or hyperbola, the tangents at the ends of a focal chord intersect on the corresponding directrix. This application of the chord of contact theorem helps in understanding the relationship between foci, directrices, and tangent lines.
Q: Can the chord of contact be used to solve optimization problems involving tangents to conic sections?
A:
Yes, the chord of contact can be a powerful tool in optimization problems. For instance, when finding the shortest or longest tangent from an external point to a conic section, the chord of contact equation can be used to set up the problem and find critical points.
Q: How can the chord of contact be used to determine if a point lies inside, on, or outside a conic section?
A:
By attempting to construct the chord of contact for a given point, you can determine its position relative to the conic section. If real tangents can be drawn (and thus a real chord of contact exists), the point is outside. If the chord of contact reduces to a point, the point lies on the conic section. If no real chord of contact can be constructed, the point is inside the conic section.
Q: What's the relationship between the chord of contact and the tangent lines drawn from an external point?
A:
The chord of contact intersects each tangent line at the point where the tangent touches the conic section. In other words, the endpoints of the chord of contact are the points of tangency for the tangents drawn from the external point.
Q: What's the significance of the chord of contact in the study of conics using homogeneous coordinates?
A:
In homogeneous coordinates, the chord of contact takes on a particularly elegant form. It becomes a linear equation in homogeneous coordinates, which simplifies many calculations and proofs in projective geometry. This representation helps in understanding the projective properties of conic sections.
Q: How does the chord of contact theorem help in understanding the properties of tangent lines to conic sections?
A:
The chord of contact theorem provides a powerful way to analyze tangent lines. It establishes a relationship between the external point, the points of tangency, and the conic section itself. This relationship can be used to derive properties of tangent lines, such as the fact that tangent lines to a parabola make equal angles with the axis and the focal radius.
Q: How can the chord of contact be used to solve problems involving the angle between tangents to a conic section?
A:
The chord of contact can be used to find the angle between tangents drawn from an external point. By using the equation of the chord of contact and the equations of the tangent lines, you can set up a system of equations to determine the angle between the tangents. This is particularly useful in problems involving orthogonal tangents.
Q: What's the relationship between the chord of contact and the concept of power of a point with respect to a conic section?
A:
The power of a point with respect to a conic section is closely related to its chord of contact. For a circle, the power of an external point is equal to the square of the length of the tangent from that point, which is also related to the position of the chord of contact. This relationship extends to other conic sections and helps in solving various geometric problems.