a treatise on the analytic geometry of three dimensions vol i 1914
TRANSCRIPT
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A
TREATISE
ON
THE ANALYTIC
GEOMETRY
OF
THREE
DIMENSIONS
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BY
THE
SAME
AUTHOR,
TREATISE
ON CONIC
SECTIONS.
CONTAINING
AN
ACCOUNT OF
SOME
OF
THE
MOST
IMPORTANT
MODERN
ALGEBRAIC
AND
GEOMETRIC
METHODS,
8vo,
125.
LONGMANS,
GREEN
AND
CO.,
LONDON,
NEW
YORK, BOMBAY, CALCUTTA,
AND
MADRAS,
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A
TREATISE
ANALYTIC
GEOMETRY
OF
THREE
DIMENSIONS
BY
GEORGE
SALMON,
D.D.,
D.C.L.,
LL.D.,
F.R.S.
LATE
PROVOST
OF TRINITY
COLLEGE,
DUBLIN
REVISED
BY
REGINALD
A.
P. ROGERS
FELLOW
OF TRINITY
COLLIiGE,
DUBLIN
SIXTH
EDITION
VOL.
I
LONGMANS,
GREEN
AND
C0.
39
PATERNOSTER
ROW,
LONDON
3
FOURTH
AVENUE
&
SOrn
STREET,
NEW
YORK
7:
BOMBAY, CALCUTTA,
AND
MADRAS
HODGES,
FIGGIS
AND
CO.,
LTD.
104
GRAFTON
STREET,
DUBLIN
1914
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EDITOR'S
PREFACE
TO FIFTH
EDITION.
VOLUME
I.
IN
order to
avoid
delay
it
has
been
thought
advisable
to
publish
this
edition
in two volumes.
While
pre-
serving
the substance
of
the fourth
edition,
I
have
added some
new matter
(generally
enclosed in
square
brackets
and
in
different
type) giving
brief
accounts
of methods
or
points
of
view
which
appear
to
me
to
be of
interest
and
to
fit
in with
the
rest
of
the
work.
The additions
include
illustrations
of
models
of
most
of the
different
species
of
quadrics,
with
gener-
ators
or lines of
curvature
(Chapter
V.)
;
articles
or
paragraphs
on
the
analytical
classification
of
real
quadrics
(880),
on
projection
and
Fiedler's
projective
coordinates
(144e),
on
the non-Eucliclean
theory
of
distance
and
angle
(144^),
and
on
the
expression
of
twisted
cubics
and
quartics
by
rational
or
eUigtic
parameters
(3330,
3470,
348,
349).-
In
differential
geometry
my
aim
has
been
to
form
a
closer
connecting-link
between
Salmon's
book
and
the more
extensive and
more
purely
analytical
methods
used
by
Bianchi,
Darboux
and others.
I
have
there-
fore
added
articles
on the
now
well-known Frenet-
Serret
formulae,
with
some
applications
(3680),
on
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vi
EDITOE'S
PEEPACE
TO
FIFTH
EDITION.
the
intrinsic
equations
of
a twisted
curve
(368J),
on
Bertrand
curves
(368c),
and
on
the
application
of
Gauss's
parametric
method
to
conformal
represent-
ation,
geodesic
curvature
and
geodesic
torsion
(3960,
3965).
To
the
portion
dealing
with
the
differential
geometry
of
curves
on
quadrics,
I have
added
Staude's
thread-construction
for
ellipsoids
(4210),
which
is
the
three-dimensional
analogue
of
Graves's
theorem
;
and
his
definitions
of confocal
quadrics
(421ft)
by
means
of
broken
distances
these
are
the
analogues
of
the
ordinary
definitions
of conies
by
means
of
focal
radii.
In
the
Golden
Age
of
Euclidean
geometry,
analogues
of
these
types
were
of
great
interest
to
men
like
Jacobi,
MacCullagh,
Chasles
and
M.
Roberts,
but
Staude's
constructions
have
virtually
brought
the
subject
to
a
conclusion.
Staude's
treatment
is
also
an excellent
illustration
of
the
elementary
and
visible
meaning
of
elliptic
and
hyper-elliptic
in-
tegrals.
New
matter
is
also
contained
in
Arts.
8Qa,
80/;,
880,
1590,
172,
173, 1760,
261,
304,
384,
and
in
various
paragraphs
throughout
the
book.
Most
of
these
additions
are
of
the
nature
of
commentaries.
About
100
examples
are
added
many
of
them
being
solved
in
order
to illustrate
the
principles
of
the
articles
to
which
they
are
appended.
The
numbering
of
the
chapters
and
of
the articles
is
the same
as in
the
fourth
edition,
except
in
Chapter
III.,
where
the
order
has been somewhat
changed,
and
in
Arts.
172,
173.
The
present
edition
has
been
published
by
the
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EDITOB'S
PBEFACE
TO
FIFTH
EDITION.
vii
direction of
the
Board
of
Trinity
College,
who
appointed
me as
Editor
in
November,
1910.
REGINALD
A.
P.
ROGERS.
TRINITY
COLLEGE,
DUBLIN,
November,
1911.
The Sixth
Edition
(1914)
of
Vol.
I.
is
reprinted
from
the
Fifth,
with
a
few
corrections,
of
which
the
most
important
are
in
Arts
88$,
338
(Ex.),
344,
357*
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PREFACE
TO
THE
THIRD
EDITION.
IN
the
preface
to
the
second
edition
of
my
Higher
Plane
Cnrres,
I
have
explained
the
circumstances
under
which
I
obtained
Professor
Cayley's
valuable
help
in
the
preparation
of
that
volume.
I
have
now
very
gratefully
to
acknowledge
that
the
same
assistance
has
been
continued
to
me in
the
re-editing
of
the
present
work.
The
changes
from
the
preceding
edition
are not
so
numerous here
as
in
the
case
of
the
Higher
Plane
Curves,
partly
because
the
book
not
having
been
so
long
out of
print required
less
alteration,
partly
because
the
size
to
which
the
volume
had
already
swelled
made
it
necessary
to
be
sparing
in
the
addition
of
new
matter.
Prof.
Cayley
having
read
all
the
proof
sheets,
the
changes
made
at
his
suggestion
are
too
numerous
to
be
particularized
;
but
the
following
are
the
parts
which,
on
now
looking
through
the
pages,
strike
me
as
calling
for
special
acknowledgment,
as
being
entirely
or
in
great
measure
derived
from
him
;
Arts.*
51-53 on
the
six
coordinates
of
a
line,
the account
of focal lines Art.
146,
Arts.f
314-322
on
Grauss's
method
of
representing
the
coordinates
of
a
point
on
a
surface
by
two
parameters.
The
discussion
of
Orthogonal
Surfaces
is
taken from
a
manuscript
memoir of
Prof.
Cayley's
Thesejarticles^have
been
altered
in
the
present
edition^
^
Arts.
377-884.
_
'
*
'
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X
PEEFACE
TO
THE
THIRD EDITION.
Arts.*
332-337
nearly
without
alteration,
and
the
following
articles
with
some modifications
of
my
own.
Prof,
Cayley
has
also
contributed
Arts, t
347
and
359
on
Curves,
Art.$
468
on
Complexes,
Arts.
567
to
the
end
of
the
chapter
on
Quartics,
and
Arts.
600
to
the
end.
Prof.
Casey
and
Prof.
Cayley
had each
supplied
me with
a
short
note
on
Cyclides,
but
I
found
the
subject
so
interesting
that
I
wished
to
give
it
fuller
treatment,
and
had
recourse
to
the
original
memoirs.
I
have
omitted
the
appendix
on
Quaternions
which
was
given
in the
former
editions,
the work of
Professors
Kelland
and
Tait
having
now
made
information
on
this
subject
very easy
to
be
obtained.
I
have
also
omitted
the
appendix
on
the order
of
Systems
of
Equations,
which has
been transferred
to
the
Treatise
on
Higher
Algebra.
I
have,
as
on
several
former
occasions,
to
acknow-
ledge help
given
me,
in
reading
the
proof
sheets,
by
my
friends
Dr.
Hart,
Mr.
Cathcart
and
Dr. Fiedler.
Owing
to
the
continued
pressure
of other
en-
gagements
I
have
been
able
to
take
scarcely
any
part
in
the
revision
of
this
fourth edition.
My
friend,
Mr.
Cathcart,
has
laid
me
under
the
great obligation
of
taking
the work
almost
entirely
oft*
my
hands,
and
it
is
at
his
suggestion
that
some
few
changes
have
been
made
from
the
last
edition.
TBINITY
COLLEGE,
DUBLIN,
Sept.,
1882.
*
Arts.
476-479
in
fourth edition.
Art.
453
in
fourth
edition,
flirts,
316
$md
328
ip
fourth
edition,
Art.
020
ip
fourth
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CONTENTS OF
VOLUME
I.
The
following
selected
course is
recommended
to
Junior
Readers
:
The
Theory
of
Surfaces
of
the
Second
Order,
Arts.
1
1446,
omitting
articles
specially
indicated in
footnotes.
Confocal
Surfaces,
Arts.
157
170.
The
Curva-
ture
of
Quadrics,
Arts.
194199.
The
General
Thewy
of
Surfaces,
Chap,
xi.
The
Theoj
y
of
Curves,
Arts.
314
323,
358376.
CHAPTER
I.
COORDINATES.
PAGE
Method of
coordinates
1
Properties
of
projections
3
Coordinates
of
point
cutting
in
a
given
ratio the
distance
between
two
points
5
Coordinates
of
centre of
a
tetrahedron
6
Distance
between
two
points
(rectangular
coordinates)
....
6
Direction-cosines,
polar
coordinates,
cylindrical
coordinates ...
7
Area
of
a
figure
in
terms
of
areas
of
its
projections
8
Angle
between
two lines in
terms of
their
direction-cosines ...
8
Perpendicular
distance
of
a
point
from
a line
......
9
Direction-cosines of
the
perpendicular
to
the
plane
of two lines
.
.
9
TRANSFORMATION
OP
COORDINATES
10
Distance between two
points
(oblique
coordinates)
..... 11
Degree
of
an
equation
unaltered
by
transformation
.....
12
CHAPTER
II.
IOTERPRETATION OP
EQUATIONS.
Meaning
of
a
single
equation
j
of
a
system
of
two
or three
equations
. 13
Every
plane
section
of
a
surface of the
n
tl1
degree
is
a
curve of the
n
th
degree
15
Every
right
line meets
a
surface of
the
h
ih
degree
in
n
points
.
. 15
Order
of
a
curve
in
space
defined
16
Three
surfaces
of
degrees
m,
n,
p
intersect
in
mnp
points
...
16
Cylindrical
surfaces
Defined
.
IT
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xii
CONTENTS.
CHAPTEB
III,
THE
PLANE
AND EIGHT
LINE.
PAGE
THE
PLANE
18
Every
equation
of the
first
degree
represents
a
plane
....
18
Equation
of
a
plane
in terms
of
its
direction-cosines and
perpendicular
from
origin
18
Angle
between
two
planes
19
Condition
that
two
planes
may
be
mutually
perpendicular
... 19
Equation
of
plane
in terms
of
intercepts
made
on
axes ....
20
Equation
of
plane
through
three points
20
Interpretation
of
terms
in
this
equation
21
Value
of
determinant
of
the
direction-cosines
of
three
right
lines
.
.
22
Length
of
perpendicular
from
a
given
point
on
a
given
plane
.
.
23
Coordinates
of
intersection
of three
planes
23
Condition
that four
planes
may
meet
in
a
point
24
Volume
of tetrahedron
in terms
of
coordinates
of
its
vertices
...
24
Volume
of
tetrahedron,
the
equations
of
whose
faces
are
given
.
.
24
Equations
of surfaces
passing
through
intersection
of
given
surfaces
,
25
The
equation
of
any
plane
can be
expressed
in
terms
of
those
of
four
given
planes
26
QtJADRIPLANAR COORDINATES,
AND
THEIR DUAL
INTERPRETATION
.
.
26
Anharmonic ratio
of
four
planes
27
General formulae for
linear
transformation of
quadriplanar
coordinates
,
28
Volume
of
tetrahedron
in
terms
of
homogeneous
coordinates
of
vertices .
29
THE
BIGHT
LINE
SO
Equations
of
a
right
line
include
four
constants
80
Condition
that
two lines
may
intersect
31
Direction-cosines
of
a
line whose
equations
are
given
.... 32
Equations
of
perpendicular
from a
given
point
on
a
given
plane
.
.
38
Direction-cosines
of
the
bisectors
of
the
angle
between
two
lines
.
.
S3
Equation
of
plane
bisecting
the
angle
between
two
given
planes
.
.
34
Angle
between
two
lines
34
Conditions
that a
line
may
lie in
a
given
plane
.
...
85
Number
of
conditions
that
a
line
may
lie
in
a
given
surface
.
.
.35
Existence
of
right
lines
on
surfaces
of
the
second
and
third
degrees
.
85
Equation
of
plane
drawn
through
a
given
line
perpendicular
to
a
given
plane
g$
Equation
of
plane
parallel
to
two
given
lines
86
Equations
and
length
of
shortest
distance
between
two
given
lines
.
38
THE Six
COORDINATES OF A
LINE
39
Identical
relation
connecting
them
40
Moment
of
two
right
lines
.
.
.
.
...
.
.
.41
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CONTENTS.
Xlll
PAGE
Homogeneous
coordinates
in
terms
of
right
line
as
ray
and
as
axis
. 41
Passage
from one
system
to the other
43
Condition
of
intersection of
right
lines
.......
4:5
Lines
meeting
four
right
lines
45
Transformation
of
homogeneous
coordinates
of line
46
SOME
PROPERTIES
OF
ETRAHEDRA
46
Relation
connecting
the
mutual distances of four
points
in
a
plane
.
46
Volume
of
a
tetrahedron
in
terms of its
edges
47
Relation
connecting
mutual distances
of
four
points
on a
sphere
.
.
48
Radius of
sphere
circumscribing
a
tetrahedron
49
Shortest
distance
between two
opposite
sides
50
Angle
of
inclination
of
two
opposite
sides
50
Examples
.
.
50
CHAPTER
IV.
PROPERTIES
OF
QUADRICS
IN GENERAL.
Number
of
conditions
necessary
to
determine a
quadric
....
51
Result
of
transformation
to
parallel
axes
52
Equation
of
tangent
plane
at
any
point
53
Equation
of
polar plane 54
Cones
defined
tangent
cone
.55
Cylinder
the
limiting
case
of
a cone
55
Locus
of
extremities
of harmonic
means
of
radii
through
a
point
.
. 55
Every
homogeneous
equation
in
03,
y,
z
represents
a
cone
whose vertex
is
the
origin
56
Polar
plane
of
a
point
with
regard
to
a
cone
57
Discriminant
of
a
quadric
;
condition
for
a cone
57
Coordinates
of
centre
59
Conditions
that
a
quadric
may
have
an
infinity
of
centres
...
59
Equation
of
diametral
plane
60
Conjugate
diameters
61
A
quadric
has
three
principal
diametral
planes
62
Formation
of
equation
representing
the
three
principal
planes
.
. 62
Similarity
of
parallel
sections
62
Rectangles
under
segments
of
intersecting
chords
proportional
to
the
rectangles
under
the
segments
of
a
pair
of
parallel
chords
.
63
Equations
of
tangent plane
and
cone,
&c.,
derived
by
JoachimsthaFs
method
^
Condition
that
a
plane
may
touch the
surface
65
Coordinates
of the
pole
of
a
given
plane
66
Condition
that
a line
may
touch
the
surface
66
This
condition
a
quadratic
function
of
the
six
coordinates
of
a line
.
67
Condition
that
point
of
intersection
of
three
planes
may
lie
on
quadric
.
67
Condition
that
line
joining
two
given points
may
lie
wholly
on
surface
.
67
Condition,
that
line
of intersection
of
two
given
planes
may
lie
wholly
on
surface
^
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XIV
CONTENTS.
PAGE
LINE
COORDINATES
AND
QUADRICS
68
Coordinates
of
polar
line
of
a
given
line 68
Condition
that a
line
may
touch
quadric
70
Determination
of
points
of
contact
of
tangent
planes
through
a
given
right
line
70
Complex
of
lines
72
Conditions
that
a
right
line
lie in
a
quadric
73
CHAPTER
V.
CLASSIFICATION
OF
QUADRICS.
Functions
of
coefficients
which
are
unaltered
by
rectangular
transfor-
mation
............
75
Discriminating
cubic
76
Cauchy's
proof
that
its
roots
are
real
77
CENTRAL
SURFACES
77
Ellipsoids
78
Hyperboloids
of one
sheet
79
Asymptotic
cones
79,
80
Hyperboloids
of
two
sheets
80
NON-CENTRAL
SURFACES
82
Paraboloids,
cylinders,
pairs
of
planes
84=
Actual
reduction
of
equation
of a
paraboloid
84
ANALYTICAL
CLASSIFICATION
OF
QUADRICS
86
CHAPTER
VI.
PROPERTIES OF
QUADRICS
DEDUCED FROM SPECIAL
FORMS
OF
THEIR
EQUATIONS.
CENTRAL SURFACES
88
Equation
referred
to
axes
88
Length
of normal
89
Sum
of
squares
of
reciprocals
of
three
rectangular
diameters
is
constant
89
Locus
of
intersection
of
three
tangent
planes
which
cut
at
right
angles
.
90
CONJUGATE
DIAMETERS
90
Sum of
squares
of
three
conjugate
diameters
is
constant
....
91
Parallelepiped
constant
whose
edges
are
conjugate
diameters
91
Sum
of
squares
of
projections
of
conjugate
diameters
constant
on
any
line
or
plane 93
Locus
of
intersection
of
tangent
planes
at
extremities
of
conjugate
diameters
93
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CONTENTS.
xv
PAGE
Quadratic
which
determines
lengths
of
axes
of
a
central
section
.
.
93
One section
through
any
semi-diameter
has
it
as
an
axis
...
94
Axes found
when
the
quadric
is
given
by
the
general
equation
. .
95
CIRCULAR
SECTIONS
96
Form
of
equations
of con
cyclic
surfaces
97
Two
circular
sections
of
opposite
systems
He
on
the
same
sphere
.
.
98
Umbilics defined
98
RECTILINEAR
GENERATORS
.
99
Two
lines
of
opposite
systems
must
intersect
101
No two
lines of the
same
system
intersect
101
Buled
surfaces
defined
103
Distinction between
developable
and
skew
surfaces
104:
A
right
line whose
motion is
regulated
by
three conditions
generates
a
surface
104
Surface
generated
by
a
line
meeting
three director
lines
....
105
Ditto,
when
lines
are
given by
their six
coordinates ....
106
Four
generators
of
one
system
cut
any
generator
of
the
other
in a
con-
stant
anharmonic
ratio
107
Surface
generated
by
lines
joining
corresponding
points
on two
homo-
graphically
divided
lines
107
NON-CENTRAL SURFACES
108
Circular
sections
of
paraboloids
108
Bight
lines on
hyperbolic paraboloid
109
Method
of
constructing
hyperbolic
paraboloid
110
Conditions
for
SURFACES
OF
BEVOLUTION
112
EXAMPLES OF
Loci
114
Orthogonal
hyperboloids,
equilateral
hyperboloids
116
Locus
of
intersection
of
three
rectangular tangent
lines
to a
quadric
.
116
Method
of
finding
equation
of
cone,
given
its
vertex,
and
a
curve
through
which
it
passes
117
Beciprocal
cones
117
CHAPTEB
VII.
RECIPROCATION,
DUALITY,
ABRIDGED
NOTATION
AND
PROJECTION.
BECIPROCATION
AND
THE
PRINCIPLE
OF DUALITY
119
Degree
of
the
reciprocal
of
a
surface,
how
measured
....
119
Beciprocal
of
a
curve
in
space
120
Osculating
plane
of
a
curve defined
120
Plane section
of
one
surface answers
to
tangent
cone
of
reciprocal
.
.
121
BECIPROOATION
WITH
REGARD
TO
SPHERE
121
Beciprocal
of
quadric,
when
ellipsoid,
hyperboloid,
or
paraboloid
. .
121
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XVI
CONTENTS.
PAGli
Reciprocal
of ruled
surface
is
ruled
surface
of
same
degree
.
. .
122
Reciprocal
cones defined
122
Sections
by
any
plane
of
reciprocal cones
are
reciprocal
....
122
Focal
lines
of
a
cone defined
122
Reciprocal
of
sphere
123
Properties
of surfaces
of
revolution
obtained
by
reciprocation
.
.
.
124
Equation
of
reciprocal
of
a
quadric
125
TANGENTIAL
EQUATIONS
126
Tangential
equation
of
a
quadric
127
ABRIDGED NOTATION
.128
Equation
of
system
of
quadrics
having
common
curve
....
129
All
quadrics
through
seven
points pass
through
an
eighth
.
.
.
130
Locus of
centres
of
quadrics
touching eight
planes
130
5J
passing
through
eight
points
.
.
.
131
Four
cones
pass
through
the
intersection
of
two
quadrics
.
. .
132
The
self
-conjugate
tetrahedron
of
two
quadrics
132
Four
conies
are
touched
by
tangent
planes
common
to two
quadrics
.
133
Properties
of
systems
of
quadrics
having
double
contact
....
133
Properties
of three
quadrics
having
one
plane
curve
common
. .
. 134
Similar
quadrics
135
Geometrical
solution
of
problem
of
circular
sections
....
135
Twelve
umbilics
lie
three
by
three
on
eight
lines
135
Definition
of
'
axes
'
and
'
perpendicular
'
by
imaginary
circle
at
infinity
136
Quadrics
touching
along
a
plane
curve
136
Properties
of
their
sections
137
Two
quadrics
having
plane
contact with
the same
third
intersect
in
plane
curves
137
Form
of
equation
referred
to
self-con
jugate
tetrahedron
....
137
Lines
joining
vertices of
tetrahedron
to
corresponding
vertices
of
polar
tetrahedron
all
generators
of
same
hyperboloid
.
.
.
.188
Analogues
of
Pascal's
theorem
142
Hexagon
of
generators
of
a
hyperboloid
142
Examples
145
PEOJEOTIVE
COOEDINATBS,
GOLLINEATION,
RBCIPKOCATION
.
.
.
145
Linear
projection
defined
146
Projection
determined
by
five
elements
and
their
correspondents
.
.
146
Euclidean
congruence
147-148
The
Euclidean
absolute
143
Generalised
congruence
and
the
absolute
148
Generalised
definition
of
distance
148
Elliptic
and
hyperbolic
spaces
149
Parabolic
space,
Euclidean
distance
150
Generalised
definition
of
angle
150
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CONTENTS.
CHAPTER
VIII.
FOCI
AND
CONFOCAL
SURFACES.
PAGE
Foci
AND
FOCAL
CONICS
(first
method)
151
Focus
and
directrix
of
a
quadric
defined
,
151
Focus
defined
as
intersection
of
two
generators
of
circumscribed
develop-
able
through
circle
at
infinity
152
Foci
in
general
lie on
a
curve
locus
153
Surfaces
when confocal
153
Tangential
equations
of
quadrics
of
confocal
system
153,
Two
kinds
of
foci
153
Focal
conies
154
Analysis
of
species
of focal
conies for
each
kind
of
quadric
. .
,
155
Foci of
sections normal
to a
focal
conic
157
Focal
lines
of a cone
157
Focal
conies
of
paraboloids
159
Focus
and
directrix
property
of
quadrics
160
Tangent
cone,
whose
vertex
is
a
focus,
is
a
right
cone
....
162
Beciprocal
of
a
quadric
with
regard
to
a
focus
is
a
surface
of
revolution
.
162
Property
of
umbilicar
foci
obtained
by
reciprocation
with
regard
to
sphere
163
Focal
properties
of
quadrics
obtained
by
reciprocation
with
regard
to
sphere
168
Spheres
of
given
radius
having
double
contact
with
quadric
. .
. 164
FOCAL CONICS AND
CONFOCAL
SURFACES
(second
method)
.
.
. 165
Focal
conies
as
limits of
quadrics
167,
Three
confocals
through
a
point
all
real
and
of different
species
.
.
167
Reciprocal
of
confocal
system
168
Coordinate's
of
intersection
of
three confocals
168
Coordinates
of
umbilics
169
Two
confocals
cut at
right
angles
169
Axes
of
central
section
in terms of
axes
of confocals
through
extremity
of
conjugate
diameter
.
170
Expression
for
length
of
perpendicular
on
tangent
plane
.
. .
171
pD
constant
along
the intersection
of
fcwo
confocals
....
172
Locus
of
pole
of fixed
plane
with
regard
to
a
system
of
confocals
.
.
173
Axes of
tangent
cone are
the
three
normals
through
its
vertex
. .
173
Transformation
of
equation
of
tangent
cone
to
the
three
normals
as
axes
of
coordinates
(three
methods)
175-177
Cones
circumscribing
confocal
surfaces
are
confocal
....
179
The
focal
lines
of
these
cones are
the
generators
of
the
hyperboloid
through
the
vertex
179
Tangent
planes through
any
line
to the
two
confocals
which
it
touches
are
mutually
perpendicular
180
Two confocals
seen from
any
point appear
to
cut
at
right
angles
.
.
180
b
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XV111
CONTENTS.
Eeal
and
apparent
intersections
of
confocals
180
Normals
to
tangent
planes
through
a
given
line
generate
a
hyperbolic
paraboloid
.
181
Chasles's
method
of
obtaining
equation
of
tangent
cone
....
183
Locus of
intersection
of
three
rectangular
planes
each
touching
a
confocal
183
Intercept
on bifocal chord
between
tangent plane
and
parallel
central
plane
184=
Given three
conjugate
diameters
of
a
quadric,
to
find
the
axes
.
.
185
Locus of
vertices
of
right
cones
enveloping
a
quadric
:
which
stand
on
given
conic
...........
186
Either of
two
focal
conies
may
be
considered
as
a
locus
of
foci
of
the
other
187
Locus
of
intersection
of
three
mutually
perpendicular
tangent
lines
,
189
Corresponding
points
on
confocals
189
Elliptic
coordinates
191
Projections
of curves
on
ellipsoid
on
planes
of
circular
section
. .
191
Ivory's
theorem
as
to
the
distance
of two
corresponding
points
.
.
192
A
mechanical
property
of
confocal
hyperboloids
of
one sheet
.
.
.
193
Jacobi's
analogue
to
the
plane
theorem
that
the
sum
of
focal
distances
is
constant
193
JbachimsthaPs
analogue
for construction
of
normals
....
194
Locus
of
points
of contact
of
parallel
planes
touching
a series
of
confocals
.
195
Purser's theorem
on
intersecting
normals
196
CURVATUEE
OF
QUADBICS
196
Eadii of
curvature
of
a
normal
and
of
an
oblique
section
....
197
Line
of
curvature defined
199
Construction
of
principal
centres
of
curvature
199
Surface
of
centres
;
its sections
by principal
planes
200
Equation
of
its
reciprocal
201
CHAPTEE
IX.
INVARIANTS
AND
COVARIANTS
OF
SYSTEMS
OF
QUADRIC8.
SYSTEM
OF
TWO
QUADEICS
202
Fundamental
invariants
of
a
system
of
two
guadrics
....
202
Geometrical
meaning
of
vanishing
of
invariants
204
Hesse's
theorem
as
to
vertices
of
two
self-conjugate
tetrahedra
.
.
204
Property
of
spheres
circumscribing
self-conjugate
tetrahedra
.
. .
205
Condition
that
two
quadrics
should
touch
,
205
Equation
of
surface
parallel
to
a
quadric
;
expressed
in
parameters
. 206
Point
of
contact of
two
surfaces,
a
double
point
on their curve
of
inter-
section
207
Stationary
contact
defined
208
Equation
of
surface
of
centres
formed
209
Surface
of
centres defined
by
two
parameters
211
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CONTENTS.
'
XIX
PAGE
Condition
that
a
tetrahedron
can be
inscribed
in
one
quadric
having
two
pairs
of
opposite
edges
on
another
211
Equation
of
quadric
touching
four
planes
212
Invariants of
a
cone
and
a
quadric
213
Two
kinds
of
equilateral hyperboloids
214
Orthogonal
hyperboloids
214
Tangential
equation
of
imaginary
circle at
infinity
215
Two
planes
at
right
angles
conjugate
with
regard
to
imaginary
circle
.
215
Tangential
equation
of
curve
in
space
.......
215
How
to
form
reciprocal
of
tangential
equation
of
a conic
. .
.
216
Equation
of
cone
touching
a
quadric
along
a
given
plane
section
.
. 216
Contravariants
of
a
system
of
two
guadrics
216
Two
principal
covariant
guadrics
of
a
system of
two
quadrics
.
. .
218
Equation
of
developable
circumscribing
two
quadrics
....
220
Its
sections
by
the
principal
planes
.
220
The
developable,
its
cuspidal
edge
and
its
tangent planes
defined
by
parameters
222
Complex
of
lines
meeting
curve
of
intersection
of two
quadrics
.
. 222
Condition
that
a
line should
be
cut
harmonically
by
two
quadrics
.
.
223
Equation
of
developable
generated
by
intersection
of
two
guadrics
.
.
223,
Intersection
of
this
developable
with
either
quadric
.....
224
Coordinates
of
a
tangent
to
the
common
curve
expressed
by
a
parameter
226
Section
of
developable
by
principal
planes
227
Coordinates
of
point
on
curve and of
osculating
plane,
how
expressed
.
228
A
system
of confocals
is
touched
by
a
common
developable
.
.
.
228
Locus
of
points
whence three
rectangular
lines
or
planes
can be
drawn
to
a
quadric
229
Two
quadrics
having
a
common
curve
can
be
described
to
touch a
line,
and
three
to
touch
a
plane 230
Properties
of confocals
deduced from
those of
a
system
inscribed
in
a
common
developable
230
Method
of
finding
equations
of
focal
conies
of
quadric
given
by
general
equation
232
Quadriplanar equation
of
system
of confocals
232
Theorems
respecting
perpendiculars,
how
generalised
....
233
Tangential equation
of
sphere
inscribed
in
a
tetrahedron
.
.
.
234
Equation
of
circumscribing
sphere
234
Conditions
that
quadriplanar
equation should
represent
a
sphere
. .
235
Condition
that
a
plane
section
should be
a
parabola
or
equilateral
hyperbola
236
Coordinates
of foci
of
a
plane
section
236
Locus
of foci of
central
section
of
a
given
quadric
237
Jacobian
of
a
system
of four
quadrics
238
Locus
of
vertices
of
cones which
pass
through
six
given
points
.
.
239
Jacobian
of
four
spheres
240
Reduction
of
two
quadrics
to
their
canonical
form
.
240
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XX
CONTENTS.
PAGE
SYSTEM
OF THBEE
QUADBICS
242
Invariants
of
a
system
of three
quadrics
242
Condition
for
three
quadrics
to
be
each
the
sum
of
five
squares
same
as
for
each to
be
polar
quadrio
of a
point
with
regard
to
a
cubic
.
243
Tact-invariants
245
Discriminants:
of
discriminants
........
246
Jacobian
curve
of
three
quadrics
246
Complex
of
lines cut in
involution
by
three
quadrics
....
247
CHAPTER
X.
CONES
AND
SPHEBO-CONICS.
A
cone
may
have sheets
of two kinds 249
Spherical
coordinates
..........
250
Protective
generalisation
of
sphero-conics
254
Cyclic
arcs
of
sphero-conics
analogous
to
asymptotes;
analogous
theorems 255
Sum
of
focal
distances
constant
........
256
Focus
and
directrix
property
of
sphero-conics
......
257
Confocal
sphero-conics
257
Any
generator
of
hyperboloid
makes
with
planes
of
circular section
angles
the
product
of
whose
sines
is
constant
258
Difference
of
squares
of
reciprocal
of axes
of
central
section
of
a
quadric,
proportional
to
product
of
sines
of
angles
it
makes
with
cyclic
planes
259
Graves
's
theorem
260
Locus of
intersection
of
rectangular
tangents
to
a
sphero-conic,
&c.
.
260
Equation
in
spherical
coordinates
of
imaginary
circle
at
infinity
.
.
261
Equation
of
sphere
inscribed
in
a
tetrahedron
262
Equation
of
a
right
cone
.........
262-263
Investigation
of
Hart's extension of
Feuerbach's
theorem
. .
. 264
Extension of
Hart's
extension
267
CHAPTER
XI.
GENERAL
THEOBY
OF
SUBFACES
(iNTBODUCTOBY
CHAPTEB),
CURVATUBE,
CHABACTEBISTICS
AND
LOCAL FOBM
OF
SUBFACES
Number of
terms in
general
equation
208
Surfaces
depending
on
one or
two
undetermined
constants
.
.
.
269
Section
of
surface
by
tangent
plane
has
point
of
contact for
a
double
point
269
A
surface
in
general
has
triple
tangent
planes,
and
an
infinity
of
double
270
Inflexional
tangents
defined
271
The
indicate
;
elliptic,
hyperbolic,
and
parabolic
points
.
.
.271
Synclastic
and
anticlastic
regions
273
Asymptotic
curves
on
a
surface
374
The
three
kinds
of
point
illustrated
by
y
i
*
?
-L
* ,
y' ,
* ',
1
Expanding
this
by
the
common
rule,
the
equation
is
+
y
{/
(a?
-
a;' )
+
*
(a;'
-
z')
+
/
(x'
-
a; )}
+
*
{x'
(if
-
y' )
+
x
(y
fff
-
?/)
+
x'
(y
f
-
y )
}
=
x'
(y z
tft
-
if'z )
+
(^'V
-
y
y )
+
a-
w
^'
-
?J
V)
.
If
we
consider
x,
y,
z
as the
coordinates
of
any
fourth
point,
we
have
the
condition
that
four points
should
lie
in
one
plane.
32.
The
coefficients
of
a?,
y,
z
in
the
preceding
equation
are
evidently
double
the
areas of the
projections
on
the
co-
ordinate
planes
of
the
triangle
formed
by
the
three
points*
If
now
we
take
the equation
(Art.
27)
x
cos
a+y
cos
/3-f
#
cos
y=p,
and
multiply
it
by
twice
A
(A
being
the
area
of
the
triangle
formed
by
the
three
points),
the
equation
will
become identical
with that
of
the last
article,
since
A
cos
a,
A
cos
/3,
A
cos
7,
are
the
projections
of
the
triangle
on
the
coordinate
plane's
(Art.
4).
The
absolute
term
then
must
be
the
same
in
both
cases.
Hence
the
quantity
%
(y * '
-
0 '* )
+
of'
(y
Y
-
Y )
+
x'
(y'z
-
#V)
represents
double the
area
of
the
triangle
formed
by
the
three
points
multiplied by
the
perpendicular
on
its
plane
from the
origin
;
or,
in
other
words,
six
times the
volume
of
the tri-
angular
pyramid^
whose base is that
triangle,
and
whose
vertex
is
the
origin.
We
can
at
once
express
A
itself
in
terms
of
the
coordi-
nates
of
the
three
points
by
Art.
12,
and
must
have
44
2
equal
to
the
sum
of
the
squares
of
the coefficients
of
x,
y,
and
#,
in
the
equation
of the
1
last
article.
Ex.
1.
To
express
the
volume
of
a
tetrahedron
in terms
of
three concur-
rent
edges
and
the
angle
between
them.
If
in
the
preceding
values we
substitute
for
x
f
,
y',
z
f
the
values
p'
cos
a',
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ANALYTIC
GEOMETBY
OF
THBEE
DIMENSIONS.
p'
cos
',
p'
cos
7',
&c.,
we find
that
six
times
the
volume
of
this
pyramid
=
p'p p (
multiplied
by
the
determinant
cos
a',
cos
',
cos
y'
cos
a ,
cos
j8 ,
cos
y
cos
a' ,
cos
|8' ,
cos
7'
Now
let
us
suppose
the
three
radii
vectores
cut
by
a
sphere
whose
radius is
unity,
having
the
origin
for its
centre,
and
meeting
it
in
a
spherical triangle
R'R'
f
R
f
.
Then
if a
denote the side
E'E ,
and
p
the
perpendicular
on
it
from
E
f
,
six
times
the
volume
of
the
pyramid
will
be
p'py
sin
a
sin
p
;
for
p'p
sin
a
is
double
the area
of
one face
of
the
pyramid,
and
p'
sin
p
is
the
perpendicular
on
it
from
the
opposite
vertex.
It
follows
then
that the
determinant
above
written
is
equal
to double
the
function
*/(sin
s sin
(5
-
a)
sin
(s
-
b)
sin
(s
-
c)J
of
the
sides
of
the
above-mentioned
spherical
triangle.
The
same
thing
may
be
proved
by forming
the
square
of
the
same
determinant
according
to
the
ordinary
rule
;
when
if
we
write
cos
a
cos
a'
+
cos
&
cos
j8'
4-
cos
7
cos
7'
=
cos
a,
&c.,
we
get
1,
cos
c,
cos
b
cos
c,
3
,
cos
a
cos
Z>,
cos
a,
1
,
which
expanded
is
1
+
2
cos
a
cos
b cos
c
-
cos
e
a
-
cos-6
-
cos-c,
which is
known
to have the value
in
question.
It is useful to
remark
that
when
the
three
lines
are at
right angles
to
each
other
the
determinant
cos
a',
cos
j3',
cos
7'
cos
a'',
cos
# ,
cos
7
cos
a' ,
cos
8' ,
cos
7'
has
unity
for
its
value.
In
fact we
see,
as
above,
that
its
square
is
1,
0,
0,
1,
0, 0,
1 .
[Ex.
2.
If the
coordinates
are
oblique
six times
the
volume
of the
pyra-
mid
is
equal
to
x',
y',
z'
x ,
?/',
*
x
f
,
y ',
z'
multiplied by
the
sine
of
the
angle
between
the
axes of
y
and
z,
multiplied
by
the sine
of
the
angle
between
the
axis
of
x
and
the
plane
of
y
s.
Ex.
3.
If the
direction
cosines
of
the
fixed axes
(oblique
or
rectangular)
re-
ferred
to
three
rectangular
axes
are
A
15
p
lt
Vl
\
A
21
/^,
v%\
A
3
,
/*.,,
y
st
prove
that
the determinant
has
the
same
value for
all
such
rectangular
axes,
and
find
its
geometrical
meaning.
(It
is the
coefficient of
the
determinant
in
Ex.
2).]
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THE PLANE
AND
THE
BIGHT
LINE.
23
33.
To
find
the
length
of
the
perpendicular
from
a
given
point x'y'z
on
a
given
plane,
x
cos
a
+
y
cos
(3+z
cos
y=p.
If
we
draw
through
x'y'z'
a
plane
parallel to
the given
plane,
and let
fall on the
two
planes
a
common
perpendicular
from
the
origin,
then
the
intercept
on
this
line
will be
equal
to
the
length
of the
perpendicular
required,
since
parallel
planes
make
equal
intercepts
on
parallel
lines.
But
the
length
of
the
perpendicular
on the
plane
through
x'y'z'
is,
by
defini-
tion
(Art.
5),
the
projection
on that
perpendicular
of the
radius
vector
to
x'y'z'
>
and
therefore
(Art.
27)
is
equal
to
x'
cos
a
+
y'
cos
ft
+
z'
cos
7.
The
length
required
is
therefore
x'
cos
a+y'
cos
/?
+
#'
cos
y
-p.
N.B.
This
supposes
the
perpendicular
on
the
plane
through
x'y'z'
to be
greater
than
p
; or,
in
other
words,
that
x'y'z'
and
the
origin
are
on
opposite
sides
of
the
plane.
If
they
were
on
the
same
side,
the
length
of
the
perpendicular
would
be
p
-
(x
f
cos
a
+
y'
cos
/5+
/
cos
7).
If the
equation
of
the
plane
had
been
given
in
the form
Ax+
By
+
Cz+
D
=
0,
it
is
reduced,
as
in Art.
28,
to
the
form
here
considered,
and
the
length
of
the
perpendicular
is
found
to
be
Ax'+By'+Cz'+D
It
is
plain
that all
points
for
which
Ax'+By'+Cz'+D
has
the same
sign
as
D,
will
be on
the same
side
of
the
plane
as
the
origin
;
and
vice
versa when the
sign
is
different.
34. To
find
the
coordinates
of
the
intersection
of
three
planes.
This
is
only
to
solve
three
equations
of
the
first
degree
for
three
unknown
quantities
(Higher
Algebra,
Art.
29,
or
Burnside
and
Panton,
Art.
144)
.
The
values
of
the
coordinates
will
become
infinite
if
the determinant
(AB'O )
vanishes,
or
A
(B'C
-
B C')
+
A'
(B C
-
BC }
+
A
(BC
r
-
B'C)
-
0.
This
then
is the
condition
that
the
three
planes
should
\>e
parallel
to
the
same
line.
For
in
such
a
case
tt^e
lii^e
of
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ANALYTIC
GEOMETRY
OF
THREE
DIMENSIONS.
intersection
of
any
two would
be also
parallel
to this
line,
and
could
not
meet the
third
plane
at
any
finite
distance.
35.
To
find
the condition
that
four
planes
should
meet
in
a
point.
This
is
evidently
obtained
by
eliminating
x,
y,
z
between
the
equations
of
the
four
planes,
and
is
therefore
the
de-
terminant
(A&CrD' ),
or
A,
B,
C,
D
A',
JB',
C
f
,
D'
\ j3 ,
C ,
D
=
0.
36.
To
find
the
volume
of
the
tetrahedron
whose
vertices
are
any
four
given
points.
If we
multiply
the area
of
the
triangle
formed
by
three
points,
by
the
perpendicular
on
their
plane
from
the
fourth,
we
obtain
three
times
the
volume.
The length
of
the
per-
pendicular
on
the
plane,
whose
equation
is
given
(Art.
31),
is
found
by
substituting
in
that
equation
the
coordinates
of the
fourth
point,
and
dividing
by
the
square
root of
the
sum
of
the
squares
of
the
coefficients
of
x,
y,
z. But
(Art.
32)
that
square
root is
double
the
area
of
the
triangle
formed
by
the
three
points.
Hence
six
times
the
volume
of
the tetrahedron
in
question
is
equal
to
the
determinant
*',
y',
*,
1
a ,
y ,
* ,
I
x'
ff
,
y' ,
*' .
1
*/' ,
y ,
* ,
1
Ex.
The
volume
of the tetrahedron
formed
by
four
planes,
whose
equa-
tions
are
given,
can be
found
by
forming
the
coordinates
of
its
angular
points,
and
then
substituting
in
the
formula
given
above. The
result
is
(HigJier
Algebra,
Art.
30,
or
Burnside or
Panton,
Art.
146),
that
six
times
the
volume
is
equal
to
_
AB'C )
(A
f
B G
fl1
)
(A B
f
C)
(
where
R
is
the
determinant
(A&C & )
t
Art.
35,
and
the
factors
in
the
de-
nominator
express
the
conditions
(Art.
34)
that
any
three
of
the
planes
should
be
parallel
to
the
same
line
f
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THE PLANE AND THE
BIGHT
LINE.
25
37.
It
is
evident,
as
In
Plane
Geometry
(see
Conies,
Art.
40),
that
if
8,
S',
8
represent
any
three
surfaces,
then
aS+
IS',
where
a
and
b
are
any
constants,
represents a
surface
passing
through
the
line
of
intersection
of
S
and 8'
;
and
that
aS
bS'+
cS
represents
a
surface
passing through
the
points
of intersection
of
S, S',
and
S .
Thus
then,
if
L, M,
N
de-
note
any
three
planes,
aL
+
bM
denotes
a
plane
passing
through
the
line of
intersection
of
the
first
two,
and
aL
+
bM
+
cN
denotes
a
plane
passing
through
the
point
common
to
all
three.*
As
a
particular
case
of
the
preceding
aL
+
b
denotes
a
plane parallel
to
Z/,
and
aL
+
bM+
c denotes
a
plane parallel
to
the
intersection
of
L
and
M
(see
Art,
30).
So
again,
four
planes
L,
M,
N,
P
will
pass
through
the
same
point
if
their
equations
are
connected
by
an identical
relation.
aL
+
bM+
cN+ dP
=
0,
for
then
any
coordinates
which satisfy
the
first
three
must
satisfy
the
fourth.
Conversely,
given
any
four
planes
inter-
secting
in a common
point,
it
is
easy
to
obtain
such
an
identical
relation.
For
multiply
the
first
equation
by
the
determinant
(A'E G
f
},
the
second
by
-
(A B' C),
the
third
by
(A^BC ),
and
the fourth
by
-
(AB'C ),
and
add,
then
(Higher Algebra,
Art.
7,
or
Burnside and
Panton,
Art.
145)
the
coefficients of
x,
y,
z
vanish
identically
;
and
the
remain-
ing
term
is the
determinant
which
vanishes
(Art.
35),
because
the
planes
meet
in
a
point.
Their
equations
are
therefore
connected
by
the
identical relation
L
(A'B C' )-~M (A B' 0)
+
N
(A^'BC')
-P
(AB'C )
=
Q.
[This
equation
may
be obtained
by
eliminating
1,
x,
y,
z,
from
the four
identical
equations
of
the
form L-D^Ax
+
By
+
Cm,
and
equating
to zero
the determinant
of
Art.
35.
By
the
same
method
it
follows
that
the
equations
of
any
*
German
writers
distinguish
the
-system
of
planes
having
a line
common
by
the name Biischel from
the
system
having
only
one
point
common,
which
they
call
BiindeL
[The
corresponding
English
terms
are
generally
pencil
and
sheaf.']
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26
ANALYTIC
GEOMETBY
OF
THBEE
DIMENSIONS.
four
planes
are
connected
by
an
identical
relation
38.
Given
any
four
planes
L,
M,
N,
P
not
meeting
in
a
point,
it
is
easy
to see
(as
at
Conies,
Art.
60)
that
the
equa-
tion
of
any
other
plane
can
be
thrown
into
the form
[This
relation
may
be
found
by
eliminating
x
9
y,
2, 1,
A:
from
the
five
equations
kL,
&c.,
where
A
=
\x
+
py
+
vz
+
p
=
0,
is
the
plane.
Thus
the
equations
of
any
five
planes
are
connected
by
a
linear
homogeneous
relation.]
In
general
the
equation
of
any
surface
of
the
degree
n
can be
expressed
by
a
homogeneous
equation
of
the
degree
n
between
L,
M,
N,
P
(see
Conies,
Art.
289),
For
the
number
of
terms
in
the
complete equation
of
the
degree
n between
three
variables
is the same
as
the
number
of terms
in
the
homogeneous
equation
of
the
degree
n between
four
variables.
Accordingly,
in
what
follows,
we shall
use
these
quadri-
planar
coordinates,
whenever
by
so
doing
our
equations
can
be
materially simplified
;
that
is,
we
shall
represent
the
equa-
tion
of
a
surface
by
a
homogeneous
equation
between
four
coordinates
x,
y,
$,
w
;
where
these
may
be
considered
as
denoting
the
perpendicular
distances,
or
quantities
propor-
tional to
the
perpendicular
distances
(or
to
given
multiples
of
the
perpendicular
distances)
of
the
point
from
four
given
planes
#
=
0,
?/
=
0,
#
=
0,
w
=
0.
It
is
at
once
apparent
that,
as
in
Conies,
Art.
70,
there is
also
a
second
system
of
interpretation
of
our
equations,
in
which
an
equation
of
the first
degree
represents
a
point,
and
the variables are the coordinates of
a
plane.
In
fact,
if
L'M'N'f denote
the
coordinates
of
a
fixed
point,
the
above
plane
passes
through
it
if
aL'+bM'+cN'+dP'=(),
and
the
coordinates of
any
plane
through
this
point
are
subject only
to
this relation.
The
quantities,
a, b,
c,
d
may
be
considere4
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THE
PLANE
AND
THE
BIGHT
LINE.
27
as
denoting
the
perpendicular
distances,
or
quantities
pro-
portional
to
the
perpendicular
distances
(or
to
given
multiples
of
the
perpendicular
distances)
of
the
plane
from
four
given
points
a
=
0,
b
=
0,
c
=
0,
d
0.
[For
the
point
whose
equation
in
plane
coordinates
is
a
=
is
the
intersection
of
the
three
planes
whose
equations
in
point
coordinates are
lf
=
0,
JV =0,
P=0;
if
we
substitute
the
coordinates
(x
l9
y
lt
^)
of
this
point
in
aL
+
bM+cN+dP
we
get
aL
lt
which
must be
proportional
to
the
perpendicular
from
x
lt
y
l9
^
on
the
plane
aL +
bM+ cN+dP
=
Q
;
hence
a
is
proportional
to
this
per-
pendicular
since L
1
is
constant.]
Ex.
1.
To
find
the
equation
of
the
plane
passing
through
x'y'z',
and
through
the
intersection
of
the
planes.
Ax
+
By
+
Cz
+
D,
A'x
+
B'y
+
C'z
+
D
f
(see
Conies,
Art.
40,
Ex?.
3).
Ans.
(A'%
1
+
B'y*
+
C'z'
+
D')(Ax
+
By
+
Ce
+
D)
=
(Ax
1
+
By'
+
C*'
4-
D)(A'x
+
B'y
4-
C's
+
')
Ex.
2.
Find
the
equation
of
the
plane
passing
through
the
points
ABC,
figure, p.
2.
The
equations
of
the
line
BC
are
evidently
~
=
1, f
+
-
=
1.
Hence
ob-
ct>
be
viously
the
equation
of
the
required
plane
is
-
+
~
+
~
=
2,
since
this
passes
CL
C
through
each
of
the
three
lines
joining
the
three
given point*.
Ex.
3. Find the
equation
of
the
plane
PEP
in
the
same
figure.
The
equations
of
the line
JEF
are x
=
0,
^
+
--
=1
;
and
forming
as
above
u C
the
equation
of
the
plane
joining
this line to
the
point abc
t
we
get
39.
If
four
planes
which
intersect in a
right
line be
met
by
any
plane,
the
anharwionic
ratio
of
the
pencil
so
formed
will
be
constant. For we
could
by
transformation of
coordinates
make the
transverse
plane
the
plane
of
xy,
and
we
should
then
obtain
the equations
of
the
intersections
of
the
four
planes
with
this
plane
by
making
#=
in the
equations.
The
resulting equations
will
be
of
the form
aL
+
M,bL
+
M,
cL
+
M,
dL
+
M
(each
equated
to
zero)
whose anharinonic
ratio
(see
Conies,
Art.
59)
depends
solely
on
the
constants
a,
6, c,
d
;
and
does
not
alter
when
by
transformation of
coordinates
L
and
M
come
to
represent
different
lines.
[This
anharmoiUQ
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28
ANALYTIC
GEOMETRY
OF THEEE DIMENSIONS.
ratio
is
evidently
the
same
as
the
anharmonic
ratio
of
the
four
points
in which
any
line
meets
the
planes.]
[Ex.
The
preceding
is
equivalent
to
the following
theorem
in
spherical
trigonometry
:
If
P,
Q,
R,
S
are
four
points
on
a
great
circle
and
any
other
point
on
the
sphere,
then
sin
PQ
sin RS
_
sin
POQ
sin
EOS
sin
PR sm
QS
~
s n~POE
sin
~QOS
where
POQ,
&c.,
represent
the
angles
between
the
great
circles
PO, OQ,
&c.]
40.
[The
homogeneous
coordinates
(x,
y,
z,
w)
of
a
point
are
linear
functions
of
its
Cartesian
coordinates
and
are
either
proportional
to
the
perpendiculars
from
the
point
on
the
faces
of
the tetrahedron
or are
proportional
to
given
multiples
of
these
perpendiculars.
If
we transform
from
the
homogeneous
coordinates
(#,
y
t
z,
w]
to another
set
(f
,
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THE
PLANE
AND
THE
EIGHT LINE. 29
It
is
evident
that
the
transformation of
coordinates is
quite
similar
for
the
coordinates
of
planes.
41.
If
we
denote
by
ax
Q9 %
,
7#
,
Sw the
perpendiculars
from
the
vertices
on the
opposite
sides of
the
original
tetra-
hedron, a,
fi,
7,
8
being
constants,
we
have
obviously,
if
Ay
By C,
D be
the
areas
of those
faces,
Aax
Q
-
Bfa
(]
=
C
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30
ANALYTIC
GEOMETRY
OF
THREE
DIMENSIONS.
to
perpendiculars
on the coordinate
planes.
Hence we
may
write
the new
coordinates
=
X
sin
p,
y
Y sin
#,
z
=
Z sin
r,
where
p,
#,
r
are
the
angles
the
axes
of
X,
1 ,
Z
make
with
the
planes
YZ,
&c.
;
therefore
x
r
,
y',
0',
1
^n
,.n
y
tr
i
y
s
}
i
ft
,*
iy
'
,,,'
^
5
if
*
j
or
by
the
relations
=
6TF
sin^
sin
q
sin
r sin
(XYZ),
y',
z',
w'
y ,
z ,
w
,
y
m
,
z
m
,
w'
sin
#
sin
r sin
(XYZ).
We
may
give
this
another
form
by
remarking
that
the
determinant
re-
duces
for
the
tetrahedron
of
reference
to
the
continued
product,
which
is
its
leading
term,
hence
^oI/oVo
=
6F?
sin^;
sin
g
sin
r
sin
(XYZ),
whence,
dividing
the
former
equation by
this,
(ayW
K
)
W
[If
a?,
y,
^,
?^
are
aw-^ homogeneous
coordinates
that
is,
any
linear
func-
tions
of
Cartesian coordinates
or
of
another
set
of
homogeneous
coordinates
-
then it
is
still
true
that
the
volume
of
the
tetrahedron
is
proportional
to
the
determinant
(X
>
IJ Z
>
IQ'
V
).
Hence
the
above
result
still
holds
good.]
The
Right
Line.
42.
The
equations
of
any
two
planes
taken
together
will
represent
their
line
of
intersection,
which
will
include
all
the
points
whose
coordinates
satisfy
both
equations. By
eliminat-
ing
x and
y
alternately
between
the
equations
we
reduce them
to
a
form
commonly
used,
viz.
The first
represents
the
projection
of
the
line
on the
plane
of
xz
and
the
second that
on
the
plane
of
yz.
The
reader will
observe
that
the
equations
of
a
right
line
imlude
four
inde-
pendent
constants.
We
might
form
independently
the
equations
of
the line
joining
two
points;
for
taking
the
values
given
(Art.
8)
of
the
coordinates of
any
point
on
that
line,
solving
for
the
ratio
m
: I
from
each
of
the
three
equations
there
given,
and
equa-
ting
results,
we
get
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THE
PLANE
AND
THE
BIGHT
LINE.
31
x -x'
__
y
j^ y^ _z
-
z
x
f
-
x
~
y
f
-
y
/f
~~
d~s{
for
the required
equations
of
the
line.
It
thus
appears
that
the
equations
of
the
projections
of
the
line
are the same as
the
equations
of
the
lines
joining
the
projections
of
two
points
on
the
line,
as
is
otherwise
evident.
43.
Two
right
lines
in