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Solid geometry (Volume 3)

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Public Domain Mark 1.0. You can find more information here.

Bibliographic data

fullscreen: Solid geometry (Volume 3)

Multivolume work

Persistent identifier:
1019887818
Author:
Reye, Theodor
Title:
Die Geometrie der Lage
Sub title:
Vorträge
Year of publication:
1868
Place of publication:
Hannover
Publisher of the original:
Rümpler
Identifier (digital):
1019887818
Language:
German
Document type:
Multivolume work

Volume

Persistent identifier:
1025709268
Author:
Reye, Theodor
Title:
Die Geometrie der Lage
Sub title:
mit einer Aufgaben-Sammlung und einer lith. Figuren-Tafel
Scope:
1 Online-Ressource (XIV, 268 Seiten, 1 ungezähltes gefaltetes Blatt)
Year of publication:
1868
Place of publication:
Hannover
Publisher of the original:
Rümpler
Identifier (digital):
1025709268
Signature of the source:
Mr.II 3000(1/2)
Language:
German
Additional Notes:
Mit einer Aufgabensammlung und einer lithografischen Figurentafel
Usage licence:
Public Domain Mark 1.0
Publisher of the digital copy:
Technische Informationsbibliothek Hannover
Place of publication of the digital copy:
Hannover
Year of publication of the original:
2018
Document type:
Volume
Collection:
Mathematics

Title page

Document type:
Multivolume work
Structure type:
Title page

Contents

Table of contents

  • Principles of geometry
  • Solid geometry (Volume 3)
  • Cover
  • Title page
  • Title page
  • PREFACE
  • "TEODORO REVE, ......, che avevo cominciato ad ammirare fin da studente, [...]
  • TABLE OF CONTENTS
  • CHAPTER I INTRODUCTION TO THE THEORY OF QUADRIC SURFACES
  • Preliminary remark.
  • Definition of a quadric surface by means of its lines.
  • The representation of this definition by means of the algebraic symbols.
  • Quadric surface defined by two conics in space having two points in common, and a line which meets these conics.
  • Definition of a quadric by two related central systems of lines and planes.
  • Quadric as representing a plane on which two fundamental points are given.
  • Consideration of the most general homogeneous equation of the second order connecting the space coordinates.
  • Consideration of particular cases. The case of a cone.
  • The case of two planes.
  • The case of two coincident planes.
  • General properties of a quadric given by its equation.
  • The polar plane of a point in regard to a quadric.
  • The tangent plane of the quadric at any point.
  • The polar line of any line in regard to a quadric.
  • The polar point, or pole, of a plane in regard to a quadric.
  • Alternative deduction of the polar point of a plane with the help of the symbols.
  • Examples of some general properties of quadrics.
  • The coordinates, and equations, of a line, in three dimensions. Elements of the theory of a linear complex.
  • CHAPTER II RELATIONS WITH A FIXED CONIC SPHERES, CONFOCAL SURFACES; QUADRICS THROUGH THE INTERSECTION OF TWO GENERAL QUADRICS
  • CHAPTER III CUBIC CURVES IN SPACE. THE INTERSECTION OF TWO OR MORE QUADRICS
  • CHAPTER IV THE GENERAL CUBIC SURFACE; INTRODUCTORY THEOREMS
  • CORRECTIONS FOR VOLUMES I AND II
  • INDEX
  • Cover

Full text

quadric 
ts if, for 
that 
esents a 
the line 
y j z > O 
quadric 
e, to the 
mch the 
quation 
lanes is 
, honio- 
quadrie 
tion for 
itaining 
itersect- 
s points 
adric in 
rie. ( )r 
ave two 
; conics, 
ì points 
a conic 
with it. 
n order 
2e ; the 
power, 
l of the 
cripti ve 
netrical 
Given 
, Draw 
ic. Let 
onic in 
te of O 
Polar plane and tangent plane defined descriptively 27 
in regard to A and B. As the line varies in this plane, passing 
through 0, the locus of P is a line, the polar line of 0 in regard to 
this conic. Now let another plane be drawn through 0, meeting 
the former plane in a line l, passing through O, and let the points 
in which the line l meets the quadric be U and V. If W be the 
harmonic conjugate of 0 in regard to U and V, the point W is on 
the polar lines of 0 in regard to both the conics, in which the 
quadric is met by the two planes drawn through 0; these two 
polar lines, therefore, intersect one another. Hence, if a third plane, 
not containing the line l, be drawn through 0, the polar line of 0, 
in regard to the conic in which this third plane cuts the quadric, 
will intersect the polar lines of 0 taken in regard to the two former 
conics, and not pass through the point of intersection of these lines, 
which is on /. The third polar line will thus lie in the plane of the 
first two. From this it is clear that, if an arbitrary line be drawn 
through 0, to meet the quadric in the points Q and R, and P be 
the point which is the harmonic conjugate of 0 in regard to Q and 
R, then the locus of P is a plane. This is called the polar plane of 
0 in regard to the quadric. From the definition it is manifest that 
if the polar plane of 0 pass through P, the polar plane of P passes 
through 0. 
The tangent plane of the quadric at any point. The polar 
plane of 0 meets the quadric in a conic. Let II be any point of 
this. Then the second point, H', in which the line OH meets the 
quadric, coincides with II; for II is the harmonic conjugate of O 
in regard to II and II'. We therefore say that the line OH touches 
the quadric at the point II. Any plane drawn through OH meets 
the quadric in a conic; this conic is met by OH in two points 
which coincide at II, that is, HO is the tangent at II of this conic. 
Again, the conic, also passing through H, in which the quadric is 
met by the polar plane of 0, has a tangent at II, say t, unless this 
conic consists of two lines. This line, t, meets the conic in two 
points which coincide at II, and, therefore, meets the quadric in 
two points which coincide at II. Consider now the conic in which 
the quadric is met by the plane containing the two lines HO and t; 
this conic is met in two points coinciding at II, both by the line 
HO and by the line t. It cannot, therefore, be a proper conic, but 
must consist of two lines meeting at II. The plane of these lines 
is called the tangent plane of the quadric at H. It is to be regarded 
as the polar plane of the point II; it passes through 0, and the 
polar plane of 0 passes through II. By choosing 0 suitably, II may 
be supposed to be any general point of the quadric. But there 
may be exception if the polar plane of 0 meets the quadric in two 
lines, as happens when the quadric degenerates into a cone, or into 
two planes; the polar plane of 0 then passes, respectively, through
	        

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Baker, Henry Frederick. Solid Geometry. University Press, 1923.
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