Equivalence of Definitions of Lemniscate of Bernoulli
Theorem
The following definitions of the concept of Lemniscate of Bernoulli are equivalent:
Geometric Definition
Let $P_1$ and $P_2$ be points in the plane such that $P_1 P_2 = 2 a$ for some constant $a$.
The lemniscate of Bernoulli is the locus of points $M$ in the plane such that:
- $P_1 M \times P_2 M = a^2$
Cartesian Definition
The lemniscate of Bernoulli is the curve defined by the Cartesian equation:
- $\paren {x^2 + y^2}^2 = 2 a^2 \paren {x^2 - y^2}$
Polar Definition
The lemniscate of Bernoulli is the curve defined by the polar equation:
- $r^2 = 2 a^2 \cos 2 \theta$
Parametric Definition
The lemniscate of Bernoulli is the curve defined by the parametric equation:
- $\begin{cases} x = \dfrac {a \sqrt 2 \cos t} {\sin^2 t + 1} \\ y = \dfrac {a \sqrt 2 \cos t \sin t} {\sin^2 t + 1} \end{cases}$
Proof
Geometric Definition equivalent to Cartesian Definition
Let $M$ be a lemniscate of Bernoulli by the geometric definition.
Then by definition:
Let $P_1$ and $P_2$ be points in the plane such that $P_1 P_2 = 2 a$ for some constant $a$.
The lemniscate of Bernoulli is the locus of points $M$ in the plane such that:
- $P_1 M \times P_2 M = a^2$
Let $P_1 = \tuple {a, 0}$ and $P_2 = \tuple {-a, 0}$.
Let $p = \tuple {x, y}$ be an arbitrary point of $M$.
We have:
\(\ds P_1 p\) | \(=\) | \(\ds \sqrt {\paren {a - x}^2 + y^2}\) | Distance Formula | |||||||||||
\(\ds \) | \(=\) | \(\ds \sqrt {a^2 - 2 a x + x^2 + y^2}\) | ||||||||||||
\(\ds P_2 p\) | \(=\) | \(\ds \sqrt {\paren {a + x}^2 + y^2}\) | Distance Formula | |||||||||||
\(\ds \) | \(=\) | \(\ds \sqrt {a^2 + 2 a x + x^2 + y^2}\) | ||||||||||||
\(\ds \leadsto \ \ \) | \(\ds \paren {P_1 p} \paren {P_2 p}\) | \(=\) | \(\ds \sqrt {a^2 - 2 a x + x^2 + y^2} \sqrt {a^2 + 2 a x + x^2 + y^2}\) | Definition of Lemniscate of Bernoulli | ||||||||||
\(\ds \) | \(=\) | \(\ds a^2\) | ||||||||||||
\(\ds \leadsto \ \ \) | \(\ds a^4\) | \(=\) | \(\ds \paren {a^2 - 2 a x + x^2 + y^2} \paren {a^2 + 2 a x + x^2 + y^2}\) | |||||||||||
\(\ds \) | \(=\) | \(\ds \paren {a^2 + \paren {x^2 + y^2} }^2 - 4 a^2 x^2\) | Difference of Two Squares | |||||||||||
\(\ds \) | \(=\) | \(\ds a^4 + 2 a^2 \paren {x^2 + y^2} + \paren {x^2 + y^2}^2 - 4 a^2 x^2\) | Square of Sum | |||||||||||
\(\ds \) | \(=\) | \(\ds a^4 + 2 a^2 \paren {y^2 - x^2} + \paren {x^2 + y^2}^2\) | simplifying | |||||||||||
\(\ds \leadsto \ \ \) | \(\ds \paren {x^2 + y^2}^2\) | \(=\) | \(\ds 2 a^2 \paren {x^2 - y^2}\) |
Thus $M$ is a lemniscate of Bernoulli by the Cartesian definition.
$\Box$
Geometric Definition equivalent to Polar Definition
Let $M$ be a lemniscate of Bernoulli by the geometric definition.
Then by definition:
Let $P_1$ and $P_2$ be points in the plane such that $P_1 P_2 = 2 a$ for some constant $a$.
The lemniscate of Bernoulli is the locus of points $M$ in the plane such that:
- $P_1 M \times P_2 M = a^2$
Let $M$ be embedded in a polar coordinate plane whose origin is at $O$ and such that $P_1 = \polar {a, 0}$ and $P_2 = \polar {a, \pi}$.
Consider an arbitrary point $p = \polar {r, \theta}$.
Let $d_1 = \size {P_1 p}$ and $d_2 = \size {P_2 p}$.
We have:
\(\ds d_1 d_2\) | \(=\) | \(\ds a^2\) | Definition of Lemniscate of Bernoulli | |||||||||||
\(\ds \) | \(=\) | \(\ds \sqrt {r^2 + a^2 - 2 a r \cos \theta} \times \sqrt {r^2 + a^2 - 2 a r \, \map \cos {\pi - \theta} }\) | Cosine Rule | |||||||||||
\(\ds \leadsto \ \ \) | \(\ds \paren {a^2}^2\) | \(=\) | \(\ds \paren {r^2 + a^2 - 2 a r \cos \theta} \paren {r^2 + a^2 + 2 a r \cos \theta}\) | Cosine of Supplementary Angle, and squaring throughout | ||||||||||
\(\ds \) | \(=\) | \(\ds \paren {r^2 + a^2}^2 - \paren {2 a r \cos \theta}^2\) | Difference of Two Squares | |||||||||||
\(\ds \) | \(=\) | \(\ds \paren {r^2}^2 + 2 a^2 r^2 + \paren {a^2}^2 - 4 a^2 r^2 \cos^2 \theta\) | ||||||||||||
\(\ds \leadsto \ \ \) | \(\ds r^2\) | \(=\) | \(\ds 2 a^2 \paren {2 \cos^2 \theta - 1}\) | simplifying and rearranging | ||||||||||
\(\ds \leadsto \ \ \) | \(\ds r^2\) | \(=\) | \(\ds 2 a^2 \cos 2 \theta\) | Double Angle Formula for Cosine: Corollary $1$ |
$\Box$
Parametric Definition equivalent to Cartesian Definition
Let $M$ be a lemniscate of Bernoulli by the parametric definition.
Then by definition:
The lemniscate of Bernoulli is the curve defined by the parametric equation:
- $\begin{cases} x = \dfrac {a \sqrt 2 \cos t} {\sin^2 t + 1} \\ y = \dfrac {a \sqrt 2 \cos t \sin t} {\sin^2 t + 1} \end{cases}$
We have:
\(\ds x^2 - y^2\) | \(=\) | \(\ds \dfrac {2 a^2 \cos^2 t} {\paren {\sin^2 t + 1}^2} - \dfrac {2 a^2 \cos^2 t \sin^2 t} {\paren {\sin^2 t + 1}^2}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \dfrac {2 a^2 \cos^2 t \paren {1 - \sin^2 t} } {\paren {\sin^2 t + 1}^2}\) | ||||||||||||
\(\text {(1)}: \quad\) | \(\ds \) | \(=\) | \(\ds \dfrac {2 a^2 \paren {1 - \sin^2 t}^2} {\paren {\sin^2 t + 1}^2}\) | Sum of Squares of Sine and Cosine |
Then:
\(\ds x^2 + y^2\) | \(=\) | \(\ds \dfrac {2 a^2 \cos^2 t} {\paren {\sin^2 t + 1}^2} + \dfrac {2 a^2 \cos^2 t \sin^2 t} {\paren {\sin^2 t + 1}^2}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \dfrac {2 a^2 \cos^2 t \paren {1 + \sin^2 t} } {\paren {\sin^2 t + 1}^2}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \dfrac {2 a^2 \paren {1 - \sin^2 t} \paren {1 + \sin^2 t} } {\paren {\sin^2 t + 1}^2}\) | Sum of Squares of Sine and Cosine | |||||||||||
\(\ds \) | \(=\) | \(\ds \dfrac {2 a^2 \paren {1 - \sin^2 t} } {\sin^2 t + 1}\) | simplifying | |||||||||||
\(\ds \leadsto \ \ \) | \(\ds \paren {x^2 + y^2}^2\) | \(=\) | \(\ds 2 a^2 \dfrac {2 a^2 \paren {1 - \sin^2 t}^2 } {\paren {\sin^2 t + 1}^2}\) | squaring both sides and extracting $2 a^2$ | ||||||||||
\(\ds \) | \(=\) | \(\ds 2 a^2 \paren {x^2 - y^2}\) | from $(1)$ |
$\blacksquare$