Orthoptic (geometry) explained

In the geometry of curves, an orthoptic is the set of points for which two tangents of a given curve meet at a right angle.

Examples:

  1. The orthoptic of a parabola is its directrix (proof: see below),

\tfrac{x2}{a2}+\tfrac{y2}{b2}=1

is the director circle

x2+y2=a2+b2

(see below),

\tfrac{x2}{a2}-\tfrac{y2}{b2}=1,a>b

is the director circle

x2+y2=a2-b2

(in case of there are no orthogonal tangents, see below),

x2/3+y2/3=1

is a quadrifolium with the polar equation

r=\tfrac{1}{\sqrt{2}}\cos(2\varphi), 0\le\varphi<2\pi

(see below).

Generalizations:

  1. An isoptic is the set of points for which two tangents of a given curve meet at a fixed angle (see below).
  2. An isoptic of two plane curves is the set of points for which two tangents meet at a fixed angle.
  3. Thales' theorem on a chord can be considered as the orthoptic of two circles which are degenerated to the two points and .

Orthoptic of a parabola

Any parabola can be transformed by a rigid motion (angles are not changed) into a parabola with equation

y=ax2

. The slope at a point of the parabola is

m=2ax

. Replacing gives the parametric representation of the parabola with the tangent slope as parameter:

\left(\tfrac{m}{2a},\tfrac{m2}{4a}\right).

The tangent has the equation

y=mx+n

with the still unknown, which can be determined by inserting the coordinates of the parabola point. One gets

y=mx-\tfrac{m2}{4a}.

If a tangent contains the point, off the parabola, then the equationy_0 = m x_0 -\frac \quad \rightarrow \quad m^2 - 4ax_0\,m + 4ay_0 = 0holds, which has two solutions and corresponding to the two tangents passing . The free term of a reduced quadratic equation is always the product of its solutions. Hence, if the tangents meet at orthogonally, the following equations hold: m_1 m_2 = -1 = 4 a y_0The last equation is equivalent toy_0 = -\frac\,, which is the equation of the directrix.

Orthoptic of an ellipse and hyperbola

Ellipse

See main article: Director circle. Let

E:\tfrac{x2}{a2}+\tfrac{y2}{b2}=1

be the ellipse of consideration.
  1. The tangents to the ellipse

E

at the vertices and co-vertices intersect at the 4 points

(\pma,\pmb)

, which lie on the desired orthoptic curve (the circle

x2+y2=a2+b2

).
  1. The tangent at a point

(u,v)

of the ellipse

E

has the equation

\tfrac{u}{a2}x+\tfrac{v}{b2}y=1

(see tangent to an ellipse). If the point is not a vertex this equation can be solved for :

y=-\tfrac{b2u}{a2v}x+\tfrac{b2}{v}.

Using the abbreviationsand the equation

{\color{blue}\tfrac{u2}{a2}=1-\tfrac{v2}{b2}=1-\tfrac{b2}{n2}}

one gets:m^2 = \frac = \frac = \frac = \frac\, .Hence and the equation of a non vertical tangent isy = m x \pm \sqrt.Solving relations for

u,v

and respecting leads to the slope depending parametric representation of the ellipse: (u,v) = \left(-\tfrac\;,\;\tfrac\right)\, . (For another proof: see .)

If a tangent contains the point

(x0,y0)

, off the ellipse, then the equationy_0 = m x_0 \pm \sqrtholds. Eliminating the square root leads tom^2 - \fracm + \frac = 0,which has two solutions

m1,m2

corresponding to the two tangents passing through

(x0,y0)

. The constant term of a monic quadratic equation is always the product of its solutions. Hence, if the tangents meet at

(x0,y0)

orthogonally, the following equations hold: m_1 m_2 = -1 = \fracThe last equation is equivalent tox_0^2+y_0^2 = a^2+b^2\, .From (1) and (2) one gets:

Hyperbola

The ellipse case can be adopted nearly exactly to the hyperbola case. The only changes to be made are to replace

b2

with

-b2

and to restrict to . Therefore:

Orthoptic of an astroid

An astroid can be described by the parametric representation\mathbf c(t) = \left(\cos^3t, \sin^3t\right), \quad 0 \le t < 2\pi.From the condition\mathbf \dot c(t) \cdot \mathbf \dot c(t+\alpha) = 0one recognizes the distance in parameter space at which an orthogonal tangent to appears. It turns out that the distance is independent of parameter, namely . The equations of the (orthogonal) tangents at the points and are respectively:\beginy &= -\tan t \left(x-\cos^3 t\right) + \sin^3 t, \\y &= \frac \left(x+\sin^3 t\right) + \cos^3 t.\endTheir common point has coordinates:\beginx &= \sin t \cos t \left(\sin t - \cos t\right), \\y &= \sin t \cos t \left(\sin t + \cos t\right).\endThis is simultaneously a parametric representation of the orthoptic.

Elimination of the parameter yields the implicit representation 2\left(x^2+y^2\right)^3 - \left(x^2-y^2\right)^2 = 0.Introducing the new parameter one gets\beginx &= \tfrac \cos(2\varphi)\cos\varphi, \\y &= \tfrac \cos(2\varphi)\sin\varphi.\end(The proof uses the angle sum and difference identities.) Hence we get the polar representationr = \tfrac \cos(2\varphi), \quad 0 \le \varphi < 2\pi of the orthoptic. Hence:

Isoptic of a parabola, an ellipse and a hyperbola

Below the isotopics for angles are listed. They are called -isoptics. For the proofs see below.

Equations of the isoptics

Parabola:The -isoptics of the parabola with equation are the branches of the hyperbolax^2-\tan^2\alpha\left(y+\frac\right)^2-\frac=0.The branches of the hyperbola provide the isoptics for the two angles and (see picture).
Ellipse:The -isoptics of the ellipse with equation are the two parts of the degree-4 curve\left(x^2+y^2-a^2-b^2\right)^2 \tan^2\alpha = 4\left(a^2y^2 + b^2x^2 - a^2b^2\right)(see picture).
Hyperbola:The -isoptics of the hyperbola with the equation are the two parts of the degree-4 curve\left(x^2 + y^2 - a^2 + b^2\right)^2 \tan^2\alpha = 4 \left(a^2y^2 - b^2x^2 + a^2b^2\right).

Proofs

Parabola:A parabola can be parametrized by the slope of its tangents :\mathbf c(m) = \left(\frac,\frac\right), \quad m \in \R.

The tangent with slope has the equation y=mx-\frac.

The point is on the tangent if and only ify_0 = m x_0 - \frac.

This means the slopes, of the two tangents containing fulfil the quadratic equation m^2 - 4ax_0m + 4ay_0 = 0.

If the tangents meet at angle or, the equation \tan^2\alpha = \left(\frac\right)^2

must be fulfilled. Solving the quadratic equation for, and inserting, into the last equation, one getsx_0^2-\tan^2\alpha\left(y_0+\frac\right)^2-\frac = 0.

This is the equation of the hyperbola above. Its branches bear the two isoptics of the parabola for the two angles and .

Ellipse:In the case of an ellipse one can adopt the idea for the orthoptic for the quadratic equationm^2-\fracm + \frac = 0.

Now, as in the case of a parabola, the quadratic equation has to be solved and the two solutions, must be inserted into the equation\tan^2\alpha=\left(\frac\right)^2.

Rearranging shows that the isoptics are parts of the degree-4 curve:\left(x_0^2+y_0^2-a^2-b^2\right)^2 \tan^2\alpha = 4\left(a^2y_0^2+b^2x_0^2-a^2b^2\right).

Hyperbola:The solution for the case of a hyperbola can be adopted from the ellipse case by replacing with (as in the case of the orthoptics, see above).

To visualize the isoptics, see implicit curve.

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