Difference between revisions of "Conic"
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+ | A second-order curve, i.e. the set of points in a (projective, affine or Euclidean) plane whose homogeneous coordinates $ x _ {0} , x _ {1} , x _ {2} $( | ||
+ | with respect to some projective, affine or Cartesian coordinate system) satisfy an equation of the second degree: | ||
+ | |||
+ | $$ | ||
+ | F ( x) \equiv \ | ||
+ | \sum _ {i, j = 0 } ^ { 2 } | ||
+ | a _ {ij} x _ {i} x _ {j} = 0,\ \ | ||
+ | a _ {ij} = a _ {ji} . | ||
+ | $$ | ||
The symmetric bilinear form | The symmetric bilinear form | ||
− | + | $$ | |
+ | \Phi ( x, \widetilde{x} ) = \ | ||
+ | \sum _ {i, j = 0 } ^ { 2 } | ||
+ | a _ {ij} x _ {i} \widetilde{x} _ {j} $$ | ||
+ | |||
+ | is called the polar form of $ F ( x) $. | ||
+ | Two points $ M ^ { \prime } = ( x _ {0} ^ \prime , x _ {1} ^ \prime , x _ {2} ^ \prime ) $ | ||
+ | and $ M ^ { \prime\prime } = ( x _ {0} ^ {\prime\prime} , x _ {1} ^ {\prime\prime} , x _ {2} ^ {\prime\prime} ) $ | ||
+ | for which $ \Phi ( x ^ \prime , x ^ {\prime\prime} ) = 0 $ | ||
+ | are said to be polar conjugates with respect to the conic. If the line $ M ^ { \prime } M ^ { \prime\prime } $ | ||
+ | intersects the conic at points $ N _ {1} , N _ {2} $ | ||
+ | and if $ M ^ { \prime } , M ^ { \prime\prime } $ | ||
+ | are polar conjugates with respect to the conic, then $ N _ {2} , N _ {2} , M ^ { \prime } , M ^ { \prime\prime } $ | ||
+ | form a harmonic quadruple. The only self-conjugate points are the points of the conic itself. The pole of a given line with respect to a conic is the point that is polar conjugate with all the points of the line. The set of points in the plane that are polar conjugate with a given point $ M ^ { \prime } $ | ||
+ | with respect to a conic is called the polar of $ M ^ { \prime } $ | ||
+ | with respect to the conic. The polar of $ M ^ { \prime } $ | ||
+ | is defined by the linear equation $ \Phi ( x, x ^ \prime ) = 0 $ | ||
+ | in the coordinates $ x _ {0} , x _ {1} , x _ {2} $. | ||
+ | If $ \Phi ( x, x ^ \prime ) \not\equiv 0 $, | ||
+ | the polar of $ M ^ { \prime } $ | ||
+ | is a straight line; if $ \Phi ( x, x ^ \prime ) \equiv 0 $, | ||
+ | the polar of $ M ^ { \prime } $ | ||
+ | is the whole plane. In this case $ M ^ { \prime } $ | ||
+ | lies on the conic and is called a singular point of the conic. If $ R = \mathop{\rm rank} ( a _ {ij} ) = 3 $, | ||
+ | the conic has no singular points and is said to be non-degenerate or to be non-decomposing (non-splitting). In the projective plane this is a real or imaginary oval. A non-degenerate conic defines a correlation on the projective plane, i.e. a bijective mapping from the set of points onto the set of lines. A tangent to a non-degenerate conic is the polar of the point of tangency. If $ R = 2 $, | ||
+ | the conic is a pair of real or imaginary straight lines intersecting at a singular point. If $ R = 1 $, | ||
+ | every point of the conic is singular and the conic itself is a pair of coincident real straight lines (a double line). The affine properties of a conic are distinguished by the specific nature of its location and by the points and lines associated with it with respect to the distinguished line $ x _ {0} = 0 $— | ||
+ | the line at infinity. A conic is of hyperbolic, elliptic or parabolic type according to whether it intersects the line at infinity $ ( \delta < 0) $, | ||
+ | does not intersect it $ ( \delta > 0) $ | ||
+ | or is tangent to it $ ( \delta = 0) $. | ||
+ | Here | ||
− | + | $$ | |
+ | \delta = \ | ||
+ | \left | | ||
− | + | \begin{array}{ll} | |
+ | a _ {11} &a _ {12} \\ | ||
+ | a _ {21} &a _ {22} \\ | ||
+ | \end{array} | ||
+ | \ | ||
+ | \right | . | ||
+ | $$ | ||
The centre of a conic is the pole of the line at infinity, a diameter is the polar of a point at infinity, an asymptote is a tangent to the conic at a point at infinity. Two diameters are conjugate with respect to the conic if their points at infinity are polar conjugates with respect to the conic. | The centre of a conic is the pole of the line at infinity, a diameter is the polar of a point at infinity, an asymptote is a tangent to the conic at a point at infinity. Two diameters are conjugate with respect to the conic if their points at infinity are polar conjugates with respect to the conic. | ||
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====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> S.P. Finikov, "Analytic geometry" , Moscow (1952) (In Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> N.V. Efimov, "A short course of analytical geometry" , Moscow (1967) (In Russian)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> S.P. Finikov, "Analytic geometry" , Moscow (1952) (In Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> N.V. Efimov, "A short course of analytical geometry" , Moscow (1967) (In Russian)</TD></TR></table> | ||
− | |||
− | |||
====Comments==== | ====Comments==== | ||
− | |||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> G. Salmon, "A treatise on conic sections" , Longman (1879)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> O. Giering, "Vorlesungen über höhere Geometrie" , Vieweg (1982)</TD></TR></table> | <table><TR><TD valign="top">[a1]</TD> <TD valign="top"> G. Salmon, "A treatise on conic sections" , Longman (1879)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top"> O. Giering, "Vorlesungen über höhere Geometrie" , Vieweg (1982)</TD></TR></table> |
Latest revision as of 17:46, 4 June 2020
A second-order curve, i.e. the set of points in a (projective, affine or Euclidean) plane whose homogeneous coordinates $ x _ {0} , x _ {1} , x _ {2} $(
with respect to some projective, affine or Cartesian coordinate system) satisfy an equation of the second degree:
$$ F ( x) \equiv \ \sum _ {i, j = 0 } ^ { 2 } a _ {ij} x _ {i} x _ {j} = 0,\ \ a _ {ij} = a _ {ji} . $$
The symmetric bilinear form
$$ \Phi ( x, \widetilde{x} ) = \ \sum _ {i, j = 0 } ^ { 2 } a _ {ij} x _ {i} \widetilde{x} _ {j} $$
is called the polar form of $ F ( x) $. Two points $ M ^ { \prime } = ( x _ {0} ^ \prime , x _ {1} ^ \prime , x _ {2} ^ \prime ) $ and $ M ^ { \prime\prime } = ( x _ {0} ^ {\prime\prime} , x _ {1} ^ {\prime\prime} , x _ {2} ^ {\prime\prime} ) $ for which $ \Phi ( x ^ \prime , x ^ {\prime\prime} ) = 0 $ are said to be polar conjugates with respect to the conic. If the line $ M ^ { \prime } M ^ { \prime\prime } $ intersects the conic at points $ N _ {1} , N _ {2} $ and if $ M ^ { \prime } , M ^ { \prime\prime } $ are polar conjugates with respect to the conic, then $ N _ {2} , N _ {2} , M ^ { \prime } , M ^ { \prime\prime } $ form a harmonic quadruple. The only self-conjugate points are the points of the conic itself. The pole of a given line with respect to a conic is the point that is polar conjugate with all the points of the line. The set of points in the plane that are polar conjugate with a given point $ M ^ { \prime } $ with respect to a conic is called the polar of $ M ^ { \prime } $ with respect to the conic. The polar of $ M ^ { \prime } $ is defined by the linear equation $ \Phi ( x, x ^ \prime ) = 0 $ in the coordinates $ x _ {0} , x _ {1} , x _ {2} $. If $ \Phi ( x, x ^ \prime ) \not\equiv 0 $, the polar of $ M ^ { \prime } $ is a straight line; if $ \Phi ( x, x ^ \prime ) \equiv 0 $, the polar of $ M ^ { \prime } $ is the whole plane. In this case $ M ^ { \prime } $ lies on the conic and is called a singular point of the conic. If $ R = \mathop{\rm rank} ( a _ {ij} ) = 3 $, the conic has no singular points and is said to be non-degenerate or to be non-decomposing (non-splitting). In the projective plane this is a real or imaginary oval. A non-degenerate conic defines a correlation on the projective plane, i.e. a bijective mapping from the set of points onto the set of lines. A tangent to a non-degenerate conic is the polar of the point of tangency. If $ R = 2 $, the conic is a pair of real or imaginary straight lines intersecting at a singular point. If $ R = 1 $, every point of the conic is singular and the conic itself is a pair of coincident real straight lines (a double line). The affine properties of a conic are distinguished by the specific nature of its location and by the points and lines associated with it with respect to the distinguished line $ x _ {0} = 0 $— the line at infinity. A conic is of hyperbolic, elliptic or parabolic type according to whether it intersects the line at infinity $ ( \delta < 0) $, does not intersect it $ ( \delta > 0) $ or is tangent to it $ ( \delta = 0) $. Here
$$ \delta = \ \left | \begin{array}{ll} a _ {11} &a _ {12} \\ a _ {21} &a _ {22} \\ \end{array} \ \right | . $$
The centre of a conic is the pole of the line at infinity, a diameter is the polar of a point at infinity, an asymptote is a tangent to the conic at a point at infinity. Two diameters are conjugate with respect to the conic if their points at infinity are polar conjugates with respect to the conic.
The metric properties of a conic are determined from its affine properties by the invariance of the distance between two arbitrary points. The diameter of a conic that is orthogonal to the conjugate diameter is an axis of symmetry of the conic and is called an axis. A directrix of a conic is the polar of a focus.
References
[1] | S.P. Finikov, "Analytic geometry" , Moscow (1952) (In Russian) |
[2] | N.V. Efimov, "A short course of analytical geometry" , Moscow (1967) (In Russian) |
Comments
References
[a1] | G. Salmon, "A treatise on conic sections" , Longman (1879) |
[a2] | O. Giering, "Vorlesungen über höhere Geometrie" , Vieweg (1982) |
Conic. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Conic&oldid=17728