Equation of Tractrix
Theorem
$x$-Axis Asymptote
Let $S$ be a cord of length $a$ situated as a (straight) line segment whose endpoints are $P$ and $T$.
Let $S$ be aligned along the $y$-axis of a cartesian plane with $T$ at the origin and $P$ therefore at the point $\tuple {0, a}$.
Let $T$ be dragged along the $x$-axis.
Cartesian Form
The equation of the tractrix along which $P$ travels is:
- $x = a \map \ln {\dfrac {a \pm \sqrt {a^2 - y^2} } y} \mp \sqrt {a^2 - y^2}$
Parametric Form
Let $S$ be a cord of length $a$ situated as a (straight) line segment whose endpoints are $P$ and $T$.
Let $S$ be aligned along the $y$-axis of a cartesian plane with $T$ at the origin and $P$ therefore at the point $\tuple {0, a}$.
Let $T$ be dragged along the $x$-axis.
Formulation 1
The equation of the tractrix along which $P$ travels can be expressed in parametric form as:
\(\ds x\) | \(=\) | \(\ds a \paren {\ln \cot \dfrac \theta 2 - \cos \theta}\) | ||||||||||||
\(\ds y\) | \(=\) | \(\ds a \sin \theta\) |
Formulation 2
The equation of the tractrix along which $P$ travels can be expressed in parametric form as:
\(\ds x\) | \(=\) | \(\ds a \paren {u - \tanh u}\) | ||||||||||||
\(\ds y\) | \(=\) | \(\ds a \sech u\) |
$y$-Axis Asymptote
Let $S$ be a cord of length $a$ situated as a (straight) line segment whose endpoints are $P$ and $T$.
Let $S$ be aligned along the $x$-axis of a cartesian plane with $T$ at the origin and $P$ therefore at the point $\tuple {a, 0}$.
Let $T$ be dragged along the $y$-axis.
Cartesian Form
The equation of the tractrix along which $P$ travels is:
- $y = a \map \ln {\dfrac {a \pm \sqrt {a^2 - x^2} } x} \mp \sqrt {a^2 - x^2}$
Parametric Form
The equation of the tractrix along which $P$ travels can be expressed in parametric form as:
\(\ds x\) | \(=\) | \(\ds a \sin \theta\) | ||||||||||||
\(\ds y\) | \(=\) | \(\ds a \paren {\ln \cot \dfrac \theta 2 - \cos \theta}\) |
Linguistic Note
The word tractrix derives from the Latin traho (trahere, traxi, tractum) meaning to pull or to drag.
The plural is tractrices.