Imaginary Straight Lines in Cartesian Coordinate System

V. Korotkiy
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引用次数: 3

Abstract

A geometric model of imaginary conjugate straight lines a~b, allowing symbolic representation of these lines on the real coordinate plane xy is considered. In order to connect the algebraic and geometric representations of imaginary straight lines, it is proposed to use the “mark” formed by orthogonal d1 ⊥ d2 and main g1~g2 directions of the elliptic involution σ in the pencil V. The specification of two pairs of pulling apart each other real straight lines d1~d2, g1~g2 passing through V, uniquely defines the elliptic involution σ in the pencil V, therefore, the V(d1 ⊥ d2, g1~g2) mark completely defines a pair of imaginary double straight lines a~b of elliptic involution σ(V), that allows consider the mark as an “image” of these imaginary straight lines. When using a mark, it is required to establish a one-to-one correspondence between complex coefficients of imaginary double straight lines equations and a graphically given mark. The direct and inverse problems are solved in this paper. The direct one is creation a mark representing imaginary straight lines, given by its own equations. The inverse one is determination of coefficients for the equations of imaginary lines defined by the mark. The essence of the direct and inverse problems consists in establishing a oneto-one correspondence between the equations of imaginary double straight elliptic involutions σ in the pencil V, and a graphically given mark containing the orthogonal and main directions of this involution. To solve both the direct and inverse problems, the Hirsch theorem (A.G. Hirsch) is used, which establishes a one-to-one correspondence between the complex Cartesian coordinates for a pair of imaginary conjugated points and real coordinates of a special “marker” symbolically representing these points. Have been considered examples of solution for geometric problems involving imaginary lines. In particular, has been solved the problem of constructing a circle passing through a given point and touching imaginary lines defined by its mark V(d1 ⊥ d2, g1~g2). Has been proposed a graphical and analytical algorithm for determining the coefficients of equations of imaginary tangents, traced to a conic section from its inner point.
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笛卡尔坐标系中的虚直线
考虑了虚共轭直线A ~b的几何模型,该模型允许这些直线在实坐标平面xy上的符号表示。为了将虚直线的代数表示和几何表示联系起来,我们提出使用铅笔V中椭圆对合σ的正交d1⊥d2和主g1~g2方向形成的“标记”。通过V的两对相互拉开的实直线d1~d2, g1~g2的规范,唯一地定义了铅笔V中的椭圆对合σ,因此,V(d1⊥d2,g1~g2)标记完全定义了一对椭圆对合σ(V)的虚双直线a~b,这使得标记可以看作是这些虚直线的“像”。在使用标记时,要求在虚双直线方程的复系数与图形给定标记之间建立一一对应关系。本文解决了正问题和逆问题。直接的一种是创造一个代表假想直线的标记,由它自己的方程给出。逆方法是确定由标记定义的虚线方程的系数。正反问题的实质在于在铅笔V上的虚双直椭圆对合σ方程与包含该对合正交方向和主方向的图形给定标记之间建立一一对应关系。为了解决正问题和逆问题,Hirsch定理(A.G. Hirsch)被使用,它建立了一对虚共轭点的复笛卡尔坐标与符号表示这些点的特殊“标记”的实坐标之间的一对一对应关系。已经被认为是涉及虚线的几何问题的解的例子。特别是,已经解决了构造一个经过给定点并接触由其标记V(d1⊥d2, g1~g2)定义的虚线的问题。提出了一种求虚切线方程系数的图解和解析算法,该虚切线从内点追踪到圆锥截面。
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