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Synthetically, a '''parabola''' is the locus of points in a plane that are equidistant from a given line (the ''directrix'') and a given point (the ''focus'').  Alternatively, a parabola is a [[conic section]] obtained as the intersection of a right circular cone with a plane parallel to a generator of the cone.
[[Image:Parabola.jpg|thumb|right|400px|<small>Parabola y = ''x''<sup>2</sup>/(2''p'') (red line). Focus F is at (0,''p''/2). Distance FP is equal to distance PABlue dashed horizontal line is directrix. </small> ]]


Let <math>d</math> be a line and <math>F</math> a point.  In the special case when <math>F</math> is a point of <math>D</math>, the "parabola" with directrix <math>D</math> and focus <math>F</math> is the line through <math>F</math> that is perpendicular to <math>D</math>In the language of conic sections, this corresponds to the case when the plane contains a generator of the cone.
A '''parabola''' is the planar [[curve]] formed by the points that lie as far from a given [[line (Euclidean geometry)|line]] (the ''directrix'') as from a given [[point (geometry)|point]] (the ''focus'')Alternatively, a parabola is the curve you get when intersecting a right circular [[cone]] with a plane parallel to a generator of the cone (a line on the cone which goes through its apex); thus, a parabola is a [[conic section]].


To avoid this degenerate case, assume that <math>F</math> does not lie in <math>D</math>, let <math>\Pi</math> be the unique plane containing <math>F</math> and <math>D</math> and let <math>P</math> be the parabola with focus <math>F</math> and directrix <math>d</math>.  The line <math>s</math> through <math>F</math> and perpendicular to <math>D</math> is called the ''axis'' of the the parabola <math>P</math> and is the unique line of symmetry of <math>P</math>. The unique point <math>V</math> of <math>s</math> that is equidistant from <math>F</math> and <math>D</math> lies on <math>P</math> and is known as the ''vertex'' of the parabola, and the distance <math>FV</math> (half the distance from <math>F</math> to <math>D</math>) is called the ''focal distance'' of the parabola.
If the focus lies on the directrix, then the "parabola" is in fact a line. In the language of conic sections, this corresponds to the case when the plane contains a generator of the cone.  


Now let <math>P'</math> be any other parabola in <math>\Pi</math> be with the same focal distance as <math>P</math>.  Let <math>F'</math> be its focus and <math>D'</math> its directrix. Then there is a unique, orientation-preserving [[rigid motion]] of <math>\Pi</math> taking <math>F</math> to <math>F'</math> and <math>D</math> to <math>D'</math> and therefore, the parabola <math>P</math> to the parabola <math>P'</math>In other words, any two parabolas with the same focal distance are congruent.
To avoid this degenerate case, we assume that the focus lies not on the directrix. The line through the focus and [[perpendicular]] to the directrix is called the ''axis'' of the parabola. It is the unique line of symmetry of the parabola. The parabola has one point that lies on the axis. This point is called the ''vertex'' of the parabola. The distance between the focus and the vertex is called the ''focal distance'' of the parabola. It is the same as the distance between the vertex and the directrix, and half the distance from the focus to the directrix.
 
The shape of a parabola is determined by the focal distance. All parabola with the same focal distance are [[congruence (geometry)|congruent]], meaning that given any parabola can be moved to any other parabola with the same focal distance by a [[rigid motion]].
 
==Parabolic mirror==
{{Image|Refl parab.png|right|350px|Fig. 2. Reflection of beam ''B'' in a parabolic mirror.}}
Parabolic mirrors concentrate incoming vertical light beams in their focus. We show this.
 
Consider in figure  2 the arbitrary  vertical light beam ''B'' (blue, parallel to the ''y''-axis) that enters the parabola and hits it at point ''P'' = (''x''<sub>1</sub>, ''y''<sub>1</sub>). The parabola (red) has focus in point ''F''. The incoming beam is reflected at ''P'' obeying the well-known law:  incidence angle is equal to angle of reflection.  The angles involved are with the line  ''APT'' which is tangent to the parabola at point ''P''. It will be shown that the reflected beam passes through ''F''.
 
Clearly &ang;''BPT'' = &ang;''APQ'' (they are vertically opposite angles). Further &ang;''APQ'' = &ang;''FPA'' because the triangles ''FPA'' and ''QPA'' are congruent and hence  &ang;''FPA''  (angle of reflection) is equal to &ang;''BPT'' (angle of incidence).
 
We prove the congruence of the triangles: By the definition of  the parabola the line segments ''FP'' and ''QP'' are of equal length, because the length of the latter segment is the distance of ''P'' to the directrix and the length of ''FP'' is the distance of ''P'' to the focus.  The point ''F'' has the coordinates (0,''f'') and the point ''Q'' has the coordinates (''x''<sub>1</sub>, &minus;''f''). The line segment ''FQ'' has the equation
:<math>
\lambda\begin{pmatrix}0\\ f\end{pmatrix} + (1-\lambda)\begin{pmatrix}x_1\\ -f\end{pmatrix}, \quad 0\le\lambda\le 1.
</math>
The midpoint ''A''  of ''FQ'' has coordinates (&lambda; = &frac12;):
:<math>
\frac{1}{2}\begin{pmatrix}0\\ f\end{pmatrix} + \frac{1}{2}\begin{pmatrix}x_1\\ -f\end{pmatrix} =
\begin{pmatrix}\frac{1}{2} x_1\\ 0\end{pmatrix}.
</math>
Hence ''A'' lies on the ''x''-axis.
The parabola has equation,
:<math>
y = \frac{1}{4f} x^2,
</math>
and the equation of the tangent at ''P'' is
:<math>
t(x) = y(x_1) + \left(\frac{dy}{dx}\right)_{x_1} (x-x_1) =
y_1 + \frac{x_1}{2f} (x-x_1)\quad \hbox{with}\quad y_1 = \frac{x_1^2}{4f}.
</math>
This line intersects the ''x''-axis at ''t'' = 0,
:<math>
0 = \frac{x_1^2}{4f} - \frac{x_1^2}{2f} + \frac{x_1}{2f} x
\Longrightarrow \frac{x_1}{2f} x = \frac{x_1^2}{4f} \Longrightarrow x = \tfrac{1}{2}x_1.
</math>
The intersection of the tangent with the ''x''-axis is the point ''A'' = (&frac12;''x''<sub>1</sub>, 0) that—as was just shown—lies on the midpoint of ''FQ''. The corresponding sides of the triangles ''FPA'' and ''QPA'' are of equal length and hence the triangles are congruent.
 
Finally, it is of interest (but unimportant for the proof) to remark that ''AP'' is orthogonal to ''FQ'' and hence that points ''F'' and ''Q'' are related by orthogonal reflection in the tangent line ''AT''.[[Category:Suggestion Bot Tag]]

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Parabola y = x2/(2p) (red line). Focus F is at (0,p/2). Distance FP is equal to distance PA. Blue dashed horizontal line is directrix.

A parabola is the planar curve formed by the points that lie as far from a given line (the directrix) as from a given point (the focus). Alternatively, a parabola is the curve you get when intersecting a right circular cone with a plane parallel to a generator of the cone (a line on the cone which goes through its apex); thus, a parabola is a conic section.

If the focus lies on the directrix, then the "parabola" is in fact a line. In the language of conic sections, this corresponds to the case when the plane contains a generator of the cone.

To avoid this degenerate case, we assume that the focus lies not on the directrix. The line through the focus and perpendicular to the directrix is called the axis of the parabola. It is the unique line of symmetry of the parabola. The parabola has one point that lies on the axis. This point is called the vertex of the parabola. The distance between the focus and the vertex is called the focal distance of the parabola. It is the same as the distance between the vertex and the directrix, and half the distance from the focus to the directrix.

The shape of a parabola is determined by the focal distance. All parabola with the same focal distance are congruent, meaning that given any parabola can be moved to any other parabola with the same focal distance by a rigid motion.

Parabolic mirror

PD Image
Fig. 2. Reflection of beam B in a parabolic mirror.

Parabolic mirrors concentrate incoming vertical light beams in their focus. We show this.

Consider in figure 2 the arbitrary vertical light beam B (blue, parallel to the y-axis) that enters the parabola and hits it at point P = (x1, y1). The parabola (red) has focus in point F. The incoming beam is reflected at P obeying the well-known law: incidence angle is equal to angle of reflection. The angles involved are with the line APT which is tangent to the parabola at point P. It will be shown that the reflected beam passes through F.

Clearly ∠BPT = ∠APQ (they are vertically opposite angles). Further ∠APQ = ∠FPA because the triangles FPA and QPA are congruent and hence ∠FPA (angle of reflection) is equal to ∠BPT (angle of incidence).

We prove the congruence of the triangles: By the definition of the parabola the line segments FP and QP are of equal length, because the length of the latter segment is the distance of P to the directrix and the length of FP is the distance of P to the focus. The point F has the coordinates (0,f) and the point Q has the coordinates (x1, −f). The line segment FQ has the equation

The midpoint A of FQ has coordinates (λ = ½):

Hence A lies on the x-axis. The parabola has equation,

and the equation of the tangent at P is

This line intersects the x-axis at t = 0,

The intersection of the tangent with the x-axis is the point A = (½x1, 0) that—as was just shown—lies on the midpoint of FQ. The corresponding sides of the triangles FPA and QPA are of equal length and hence the triangles are congruent.

Finally, it is of interest (but unimportant for the proof) to remark that AP is orthogonal to FQ and hence that points F and Q are related by orthogonal reflection in the tangent line AT.