11
Chapter 3 Solid geometry and Desargues’ Theorem Math 4520, Fall 2017 3.1 The extended Euclidean 3-space We can regard the Euclidean plane as defined as the set of ordered pairs of real numbers. In this approach the coordinate system becomes part of the definition. Similarly, Euclidean space can be regarded as the set of ordered triples of real numbers. Then it is easy to define points, lines, and planes as solutions to linear equations. The properties of the incidence relations become a bit more complicated. A point may lie in (be incident to) a line or a plane, but a line and a plane may intersect in a point, or the line may be completely contained in plane. There are many other cases to consider as well. In any case we can add a plane of points and lines at infinity to get the extended Euclidean 3-space, just as we did to the Euclidean plane to get the extended Euclidean plane. Here are the elements (points, lines, and planes) of extended Euclidean 3-space other than the ordinary points of Euclidean 3-space. A point at infinity is identified with an equivalence class of parallel lines in Euclidean 3-space. A line at infinity is identified with an equivalence class of parallel planes in Euclidean 3-space. The plane at infinity is one additional plane that is incident to all the points and lines at infinity. It will be an exercise to provide the appropriate definitions telling when two elements are incident. This is a little like playing God. Try not to abuse the privilege. It will also be left as an exercise to create a reasonable set of axioms for projective 3-space. Note that the extended Euclidean 3-space that you finish defining must at least satisfy your set of axioms. Indeed we want to have some basic properties to be able to work in projective 3-space. For example we need to be able to define “projection”. The following is some motivation for this idea. Suppose that an artist wants to draw some object, even an object in a plane. How is this done accurately? Imagine the artist’s canvas as a transparent plane with the object on the other side from the artist’s eye. Call the artist’s eye (we ignore binocular vision) the station point or the center of projection. If the object to be drawn lies in a plane itself, we call that 1

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Page 1: Chapter 3 Solid geometry and Desargues’ Theorempi.math.cornell.edu/~web4520/CG3-0.pdf · Solid geometry and Desargues’ Theorem Math 4520, Fall 2017 3.1 The extended Euclidean

Chapter 3

Solid geometry and Desargues’TheoremMath 4520, Fall 2017

3.1 The extended Euclidean 3-space

We can regard the Euclidean plane as defined as the set of ordered pairs of real numbers.In this approach the coordinate system becomes part of the definition. Similarly, Euclideanspace can be regarded as the set of ordered triples of real numbers. Then it is easy to definepoints, lines, and planes as solutions to linear equations.

The properties of the incidence relations become a bit more complicated. A point may liein (be incident to) a line or a plane, but a line and a plane may intersect in a point, or theline may be completely contained in plane. There are many other cases to consider as well.In any case we can add a plane of points and lines at infinity to get the extended Euclidean3-space, just as we did to the Euclidean plane to get the extended Euclidean plane. Hereare the elements (points, lines, and planes) of extended Euclidean 3-space other than theordinary points of Euclidean 3-space.

A point at infinity is identified with an equivalence class of parallel lines in Euclidean3-space.

A line at infinity is identified with an equivalence class of parallel planes in Euclidean3-space.

The plane at infinity is one additional plane that is incident to all the points and lines atinfinity.

It will be an exercise to provide the appropriate definitions telling when two elements areincident. This is a little like playing God. Try not to abuse the privilege. It will also beleft as an exercise to create a reasonable set of axioms for projective 3-space. Note that theextended Euclidean 3-space that you finish defining must at least satisfy your set of axioms.Indeed we want to have some basic properties to be able to work in projective 3-space. Forexample we need to be able to define “projection”. The following is some motivation for thisidea.

Suppose that an artist wants to draw some object, even an object in a plane. How is thisdone accurately? Imagine the artist’s canvas as a transparent plane with the object on theother side from the artist’s eye. Call the artist’s eye (we ignore binocular vision) the stationpoint or the center of projection. If the object to be drawn lies in a plane itself, we call that

1

Page 2: Chapter 3 Solid geometry and Desargues’ Theorempi.math.cornell.edu/~web4520/CG3-0.pdf · Solid geometry and Desargues’ Theorem Math 4520, Fall 2017 3.1 The extended Euclidean

2CHAPTER 3. SOLID GEOMETRYANDDESARGUES’ THEOREMMATH 4520, FALL 2017

Math 452, Spring 2002R. Connelly

CLASSICAL GEOMETRIES

4. Solid geometry and Desargues' Theorem

4.1 The extended Euclidean 3-space

We can regard the Euclidean plane as defined as the set of ordered pairs of real num-

bers. In this approach the coordinate system becomes part of the definition. Similarly,

Euclidean space can be regarded as the set of ordered triples of real numbers. Then it

is easy to define points, lines, and planes as solutions to linear equations.

The properties of the incidence relations become a bit more complicated. A point

may lie in (be incident to) a line or a plane, but a line and a plane may intersect in a

point, or the line may be completely contained in plane. There are many other cases to

consider as well. In any case \ve can add a plane of points and lines at infinity to get the

extended Euclidean 3-space, just as \ve did to the Euclidean plane to get the extended

Euclidean plane. Here are the elements (points, lines, and planes) of extended Euclidean

3-space other than the ordinary points of Euclidean 3-space.A point at infinity is identified \vith an equivalence class of parallel lines in Euclidean

3-space .A line at infinity is identified \vith an equivalence class of parallel planes in Euclidean

3-space.The plane at infinity is one additional plane that is incident to all the points and lines

at infinity.It \vill be an exercise to provide the appropriate definitions telling \vhen t\VO elements

are incident. This is a little like playing God. Try not to abuse the privilege. It \vill

also be left as an exercise to create a reasonable set of axioms for projecti\,e 3-space.

Note that the extended Euclidean 3-space that )'OU finish defining must at least satisfy

)'our set of axioms. Indeed \ve \vant to ha\'e some basic properties to be able to \vork inprojective 3-space. For example \ve need to be able to define "projection " .The follo\ving

is some motivation for this idea.

2008

Figure 3.1

plane the object plane. See Figure 3.1. For every point p in the object plane consider theline through (incident to) it and the station point. This line will intersect the picture planeat a unique point q. (q will be the unique point incident to the picture plane and the line.)We say that q is the projection of p, (from the station point). We regard q as a function of pand indeed we write q = f(p). So f is a function whose domain is the set of points incidentto the object plane and whose range is the set of points incident to the picture plane. Wecall f a projection from the object plane to the picture plane.

Notice that our definition of a projection is purely formal. All we need is two distinctplanes, one we can call the object plane and the other we can call the picture plane. Ofcourse we must also be careful to choose the center of projection so that it is not incident toeither of these planes. In the extended Euclidean 3-space, as well as your generally definedprojective 3-space, any line through (incident to) the center of projection must intersect eachof the the planes in a unique point. (The line must be incident to a unique point which isalso incident to each of the two planes.) So projection is well-defined.

Here are some simple observations:

1. The projection of a line is a line. (The projection of the points incident to a line inthe object plane is the set of points incident to a line in the picture plane.) Henceprojection can be equivalently regarded as a function taking the lines of the objectplane to the lines of the picture plane.

2. Projection is a one-to-one and onto function.

3. In your extended Euclidean 3-space model, the projection of the line at infinity of theobject plane can be an ordinary line in the picture plane. You can draw a picture ofthe horizon.

The creation of the projective plane is great, but what can you do with it? Can youprove anything? This is a silly question for a mathematician, who can prove somethingabout anything. But honestly it is difficult to prove something interesting using just the barebones three axioms of the projective plane. However, if one uses projective 3-space, then itis possible to prove some remarkable statements that are intimate with the whole foundationof Geometry.

It is useful to have one other little Lemma with regard to Axiom 3 for the projectiveplane.

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3.1. THE EXTENDED EUCLIDEAN 3-SPACE 3

CLASSICAL GEOMETRIES

Suppose that an artist ,,'ants to dra,v some object, e,'en an object in a plane. Ho,,' is

this done accurately? Imagine the artist's canvas as a transparent plane ,vith the object

on the other side from the artist's eye. Call the artist's eye (we ignore binocular vision)

the station point or the center of projection. If. the object to be dra,vn lies in a plane

itself, ,ve call that plane the object plane. See Figure 4.1.1. For every point p in the

object plane consider the line through ( incident to) it and the station point. This line

,vill intersect the picture plane at a unique point Q. ( q ,vill be the unique point incident

to the picture plane and the line.) We say that q is the projection ofp, (from the station

point). We regard q as a function of p and indeed ,ve ,vrite q = f(p ). So f is a function

'v hose domain is the set of points incident to the object plane and 'v hose range is the set

of points incident to the picture plane. We call f a projection from the object plane to

the picture plane.Notice that our definition of a projection is purely formal. All ,ve need is t'vo distinct

planes, one ,ve can call the object plane and the other ,ve can call the picture plane. Of

course ,ve must also be careful to choose the center of projection so that it is not incident

to either of these planes. In the extended Euclidean 3-space, as ,vell as your generally

defined projective 3-space, an)' line through (incident to) the center of projection must

intersect each of the the planes in a unique point. (The line must be incident to a unique

point ,vhich is also incident to each of the t'vo planes. ) So projection is ,vell-defined.

Here are some simple observations:

1. The projection of a line is a line. (The projection of the points incident to a line

in the object plane is the set of points incident to a line in the picture plane.)

Hence projection can be equivalently regarded as a function taking the lines of

the object plane to the lines of the picture plane.

2. Projection is a one-to-one and onto function.

3. In your extended Euclidean 3-space model, the projection of the line at infinity

of the object plane can be an ordinary line in the picture plane. You can dra,v a

picture of the horizon.

FIGURE 4.2.1

The creation of the projective plane is great, but ,v hat can you do ,vith it? Can you

prove anything? This is a silly question for a mathematician, 'v ho can prove something

about anything. But honestly it is difficult to prove something interesting using just the

bare bones three axioms of the projective plane. However, if one uses projective 3-space,

Figure 3.2

Lemma 3.1.1. In a projective plane (or our projective space), every line is incident to atleast three distinct points (or dually every point is incident to at least three lines).

Proof. Recall that Axiom 3 holds and letL be any line. Then there are four distinct pointsp0,p1,p2,p3 in the projective plane, no three collinear. Without loss of generality we canassume that p0 is not incident to L. Then the projection from p0 of p1,p2,p3 into L are thethree required points. See Figure 3.3.

L

pp

p

32

1

0p

Figure 3.3

To properly state one very basic result, we start with a few definitions. We say that theordered triple of points [p1,p2,p3] is a point triangle if the points are not incident to anyline. Similarly, and ordered triple of lines [L1, L2, L3] is a line triangle if the three lines arenot incident to a point. Note that to each point triangle [p1,p2,p3] we can associate a linetriangle [L1, L2, L3], where L3 is the unique line incident to p1 and p2, L2 is the unique lineincident to p1 and p3, etc. See Figure 3.4. Often we will simply say “triangle” where we willmean one of these two definitions.

Suppose [p1,p2,p3] = 41 and [q1,q2,q3] = 42 are two point triangles. We say that 41

and 42 are in perspective with respect to a point p (and p is the point of perspectivity) if thelines determined by corresponding points are all incident to p. In other words, p, pi, andqi are colinear (all incident to a line), for i = 1, 2, 3. See Figure 3.5. Similarly, we say thattwo (line) triangles are in perspective with respect to a line L, if the three points incident tocorresponding lines all are incident to L.

Note that corresponding elements in these definitions (for example p1 and q1) must bedistinct in order for there to be a unique element (a line for example) determined by them.We can now state a Theorem due to Desargues, who was an architect at Lyon, France in theseventeenth century.

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4CHAPTER 3. SOLID GEOMETRYANDDESARGUES’ THEOREMMATH 4520, FALL 2017

SOLID GEOMETRY AND DESARGUES' THEOREM 3

then it is possible to prove some remarkable statements that are intimate "ith the "hole

foundation of Geometry.

To properly state one very basic result, '"e start with a fe", definitions. "re say that

the ordered triple of points [PI, P2 , P3] is a point triangle if the points are not incident to

any line. Similarly, and ordered triple of lines [£1, £2, £3] is a line triangle if the three

lines are not incident to a point. N ote that to each point triangle [p I , P2 , P 3] "'e call

associate a line triangle [Ll, £2, £3], ",here £3 is the unique line incident to PI and P2,

£2 is the unique line incident to PI and P3, etc. See Figure 4.3.1. Often ",e ",ill simply

say "triangle" ,yhere 'ye ,yill mean one of these t'YO definitions.

Suppose [Pl~P2,P3] = 61 and [ql,q2.q3] = 62-are t\VO point triangles. "re sa)' that

61 and 62 are in perspective with respect to a point P ( and P is the point of perspecti'uity)

if the lines determined b)' corresponding points are all incident to p. In other \vords, P,

Pi, and qi are colinear (all incident to a line), for i = I, 2, 3. See Figure 4.3.2. similarl~'.

\ve say that t\VO (line) triangles are in perspective with respect to a line L, if the three

points incident to corresponding lines all are incident to L.

~ (/""' p 3

L3Point of perspectivity

L2

JK-

FIGURE 4.3.2

Note that corresponding elements in these definitions (for example PI and qI) must

be distinct in order for there to be a unique element ( a line for example) determined by

them. We can no'v state a Theorem due to Desargues, ,v ho ,vas an architect at Lyon,

France in the seventeenth century.

Figure 3.4

SOLID GEOMETRY AND DESARGUES' THEOREM 3

then it is possible to prove some remarkable statements that are intimate "ith the "hole

foundation of Geometry.

To properly state one very basic result, '"e start with a fe", definitions. "re say that

the ordered triple of points [PI, P2 , P3] is a point triangle if the points are not incident to

any line. Similarly, and ordered triple of lines [£1, £2, £3] is a line triangle if the three

lines are not incident to a point. N ote that to each point triangle [p I , P2 , P 3] "'e call

associate a line triangle [Ll, £2, £3], ",here £3 is the unique line incident to PI and P2,

£2 is the unique line incident to PI and P3, etc. See Figure 4.3.1. Often ",e ",ill simply

say "triangle" ,yhere 'ye ,yill mean one of these t'YO definitions.

Suppose [Pl~P2,P3] = 61 and [ql,q2.q3] = 62-are t\VO point triangles. "re sa)' that

61 and 62 are in perspective with respect to a point P ( and P is the point of perspecti'uity)

if the lines determined b)' corresponding points are all incident to p. In other \vords, P,

Pi, and qi are colinear (all incident to a line), for i = I, 2, 3. See Figure 4.3.2. similarl~'.

\ve say that t\VO (line) triangles are in perspective with respect to a line L, if the three

points incident to corresponding lines all are incident to L.

~ (/""' p 3

L3Point of perspectivity

L2

JK-

FIGURE 4.3.2

Note that corresponding elements in these definitions (for example PI and qI) must

be distinct in order for there to be a unique element ( a line for example) determined by

them. We can no'v state a Theorem due to Desargues, ,v ho ,vas an architect at Lyon,

France in the seventeenth century.

Figure 3.5

Theorem 3.1.2 (Desargues). Two triangles are in perspective with respect to a point if andonly if they are in perspective with respect to a line.

Desargues of course only meant his Theorem to apply to the extended Euclidean plane.But the statement makes sense in any projective plane since it is only concerned with inci-dence relations. In general, the above statement is not true for all projective planes. However,we shall give a proof below that applies when the projective plane is part of a projective 3-space. This is certainly true of the extended Euclidean plane. Note also that we need onlyto prove the “only if” part of the statement, since if we reverse the words “point” and “line”and apply the same proof that will prove the “if” part of the statement.

Proof of Desargues’ Theorem. We shall first generalize the statement of Desargues’ Theoremto include the cases when the two triangles are in a projective 3-space, not just necessarily ina projective plane. You should check that the definitions of being in perspective with respectto a point or to a line apply equally well in the projective 3-space.

Start with the three coordinate axes.Consider two point triangles, where each triangle has one vertex on each axis as in 3.7.

These two shaded triangles are in perspective with respect to a point (the origin in our case).

Since the four points of the two triangles all lie on the y and z axes, they all lie in theshaded plane, the yz–plane as in Figure 3.8. Thus the corresponding sides (when extendedin this picture) are incident to a point in the yz–plane (a black dot in Figure 3.8).

Page 5: Chapter 3 Solid geometry and Desargues’ Theorempi.math.cornell.edu/~web4520/CG3-0.pdf · Solid geometry and Desargues’ Theorem Math 4520, Fall 2017 3.1 The extended Euclidean

3.1. THE EXTENDED EUCLIDEAN 3-SPACE 5

CLASSICAL GEOMETRIES4

Theorem (Desargues) : Two triangles are in perspective with respect to a point if and

only if they are in perspective with respect to a line.

Desargues of course only meant his Theorem to apply to the extended Euclidean plane .

But the statement makes sense in any projective plane since it is only concerned ,vith

incidence relations. In general, the above statement is not true for all projective planes.

Ho,yever, ,ye shall give a proof below that applies ,yhen the projective plane is part of

a projective 3-space. This is certainly true of the extended Euclidean plane. Note also

that ,ye need only to prove the "only if' part of the statement, since if ,ve reverse the

,yords "point" and "line" and apply the same proof that ,vill prove the "if' part of the

statement.

Proof of Desargues ' Theorem: We shall first generalize the statement of Desargues' The-

orem to include the cases 'v hen the t'vo triangles are in a projective 3-space, not just

necessarily in a projective plane. You should check that the definitions of being in per-

spective with respect to a point or to a line apply equally "ell in the projective 3-space.

Start \\ith the three coordinate axes

Consider t\VO point triangles, \V here each triangle has one vertex on each axis. T'hese

rn-o shaded triangles are in perspective \vith respect to a point (the origin in our case).

Figure 3.6

CLASSICAL GEOMETRIES4

Theorem (Desargues) : Two triangles are in perspective with respect to a point if and

only if they are in perspective with respect to a line.

Desargues of course only meant his Theorem to apply to the extended Euclidean plane .

But the statement makes sense in any projective plane since it is only concerned ,vith

incidence relations. In general, the above statement is not true for all projective planes.

Ho,yever, ,ye shall give a proof below that applies ,yhen the projective plane is part of

a projective 3-space. This is certainly true of the extended Euclidean plane. Note also

that ,ye need only to prove the "only if' part of the statement, since if ,ve reverse the

,yords "point" and "line" and apply the same proof that ,vill prove the "if' part of the

statement.

Proof of Desargues ' Theorem: We shall first generalize the statement of Desargues' The-

orem to include the cases 'v hen the t'vo triangles are in a projective 3-space, not just

necessarily in a projective plane. You should check that the definitions of being in per-

spective with respect to a point or to a line apply equally "ell in the projective 3-space.

Start \\ith the three coordinate axes

Consider t\VO point triangles, \V here each triangle has one vertex on each axis. T'hese

rn-o shaded triangles are in perspective \vith respect to a point (the origin in our case).Figure 3.7

Similarly for the other two sides (when extended), we obtain two more points as in Figure3.9.

But each of these points (the black dots) is incident to one (extended) side of each triangle.So they are all incident to both planes of the two triangles we started with. Hence these threepoints are incident to the line of intersection (incident to) the planes of those triangles as inFigure 3.10.

So the two triangles are in perspective with respect to a line, which finishes Desargues’Theorem. . . . Or does it? We neglected to consider the case when the two triangles (or moreprecisely the points and lines of these two triangles) are both incident to the same plane,which is precisely the case we started with. But we can save things if we can project thepoints and lines in projective 3-space in such a picture as above into any given configuration(a collection of points and lines) in the projective plane. We do that as follows.

Start with the two triangles that are incident to the same plane as in 3.11. We assumethat these two triangles are also in perspective with respect to a point in that plane.

Choose a new point not incident to this plane. Regard this new point as a point of

Page 6: Chapter 3 Solid geometry and Desargues’ Theorempi.math.cornell.edu/~web4520/CG3-0.pdf · Solid geometry and Desargues’ Theorem Math 4520, Fall 2017 3.1 The extended Euclidean

6CHAPTER 3. SOLID GEOMETRYANDDESARGUES’ THEOREMMATH 4520, FALL 2017SOLID GEOMETRY A:\,D DESARGUES' THEOREM 5

Since the four points of the t'vo triangles all lie on the y and z axes. they all lie in

the shaded plane, the yz-plane. Thus the corresponding sides (,vhen extended in this

picture) are incident to a point in the y ::-plane ( a black dot in the above picture) .

But each of these points ( the black dots) is incident to one ( extended) side of each

shaded triangle. So they are all incident to both planes of the shaded triangles. Hence

these three points are incident to the line of intersection (incident to) the planes of the

shaded triangles.

Figure 3.8

SOLID GEOMETRY A:\,D DESARGUES' THEOREM 5

Since the four points of the t'vo triangles all lie on the y and z axes. they all lie in

the shaded plane, the yz-plane. Thus the corresponding sides (,vhen extended in this

picture) are incident to a point in the y ::-plane ( a black dot in the above picture) .

But each of these points ( the black dots) is incident to one ( extended) side of each

shaded triangle. So they are all incident to both planes of the shaded triangles. Hence

these three points are incident to the line of intersection (incident to) the planes of the

shaded triangles.

Figure 3.9

projection from projective 3-space into the given plane as in Figure 3.12.

Choose another point (in black in Figure 3.13) incident to the line incident to the pointof projection and the point of perspectivity in the plane. This new point will be the point ofperspectivity in projective 3-space, and it must be chosen not equal to the point of projectionor the point of perspectivity in the plane. This can be done by using Lemma 3.1.1. Nextchoose the point indicated in Figure 3.13, that will be the corresponding point of the newtriangle.

Do the same for all three pairs of corresponding points as in Figure 3.14.Now we can really project the configuration in projective 3-space into the plane of one

of the triangles, and we have shown that the two triangles are in perspective with respect tosame line of perspectivity. This finishes our “proof” of Desargues’ Theorem.

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3.1. THE EXTENDED EUCLIDEAN 3-SPACE 7

SOLID GEOMETRY A:\,D DESARGUES' THEOREM 5

Since the four points of the t'vo triangles all lie on the y and z axes. they all lie in

the shaded plane, the yz-plane. Thus the corresponding sides (,vhen extended in this

picture) are incident to a point in the y ::-plane ( a black dot in the above picture) .

But each of these points ( the black dots) is incident to one ( extended) side of each

shaded triangle. So they are all incident to both planes of the shaded triangles. Hence

these three points are incident to the line of intersection (incident to) the planes of the

shaded triangles.

Figure 3.10

6CLASSICAL GEO~IETRIES

So the t'vo triangles are in perspective ,vith respect to a line, ,vhich finishes Desargues.

Theorem. ...Or does it? We neglected to consider the case ,vhen the t'vo triangles

( or more precisely the points and lines of these t"'O triangles) are both incident to the

same plane, ,vhich is precisely the case ,ve started with. But ,ve can save things if ,ve

can project the points and lines in projective 3-space in such a picture as above into any

gi,'en configuration ( a collection of points and lines) in the projecti,'e plane. \\le do thatas follows.

Start with the t,"o triangles that are incident to the same plane. We assume that

these two triangles are also in perspective ,vith respect to a point in that plane.

Choose a ne,v point not incident to this plane. Regard this ne,v point as a point of

projection from projective 3-space into the gi\ell plane.

Choose another point (in black belo\v) on the line through the point of projection and

the point of perspectivity in the plane. This ne,v point \vill be the point of perspectivity

in projective 3-space, and it must be chosen not equal to the point of projection or the

point of perspecti"ity in the plane. Kext choose the point indicated belo\v, that \vill be

the corresponding point of the ne\v triangle.

Figure 3.11

6CLASSICAL GEO~IETRIES

So the t'vo triangles are in perspective ,vith respect to a line, ,vhich finishes Desargues.

Theorem. ...Or does it? We neglected to consider the case ,vhen the t'vo triangles

( or more precisely the points and lines of these t"'O triangles) are both incident to the

same plane, ,vhich is precisely the case ,ve started with. But ,ve can save things if ,ve

can project the points and lines in projective 3-space in such a picture as above into any

gi,'en configuration ( a collection of points and lines) in the projecti,'e plane. \\le do thatas follows.

Start with the t,"o triangles that are incident to the same plane. We assume that

these two triangles are also in perspective ,vith respect to a point in that plane.

Choose a ne,v point not incident to this plane. Regard this ne,v point as a point of

projection from projective 3-space into the gi\ell plane.

Choose another point (in black belo\v) on the line through the point of projection and

the point of perspectivity in the plane. This ne,v point \vill be the point of perspectivity

in projective 3-space, and it must be chosen not equal to the point of projection or the

point of perspecti"ity in the plane. Kext choose the point indicated belo\v, that \vill be

the corresponding point of the ne\v triangle.

Figure 3.12

Page 8: Chapter 3 Solid geometry and Desargues’ Theorempi.math.cornell.edu/~web4520/CG3-0.pdf · Solid geometry and Desargues’ Theorem Math 4520, Fall 2017 3.1 The extended Euclidean

8CHAPTER 3. SOLID GEOMETRYANDDESARGUES’ THEOREMMATH 4520, FALL 2017

SOLID GEOMETRY A:-.:D DESARGUES' THEOREM

Do the same for all three pairs of corresponding points as belo\v

Point ofn projection

Point of

Correspondingpoints of the new

triangle

No,,' ,ve can project the configuration in projective 3-space into the plane of one of

the triangles, and ,ve ha,'e sho,vn that the t'vo triangles are in perspective ,vith respect

to same line of perspectivity. This finishes our ..proof' of Desargues' Theorem.

Figure 3.13

SOLID GEOMETRY A:-.:D DESARGUES' THEOREM

Do the same for all three pairs of corresponding points as belo\v

Point ofn projection

Point of

Correspondingpoints of the new

triangle

No,,' ,ve can project the configuration in projective 3-space into the plane of one of

the triangles, and ,ve ha,'e sho,vn that the t'vo triangles are in perspective ,vith respect

to same line of perspectivity. This finishes our ..proof' of Desargues' Theorem.

Figure 3.14

Page 9: Chapter 3 Solid geometry and Desargues’ Theorempi.math.cornell.edu/~web4520/CG3-0.pdf · Solid geometry and Desargues’ Theorem Math 4520, Fall 2017 3.1 The extended Euclidean

3.2. EXERCISES: 9

3.2 Exercises:

1. Complete the definition of the extended Euclidean 3-space.

2. Finish the definition of projective 3-space so that the above proof of Desargues’ Theoremis valid. You may only include axioms that are valid for the extended Euclidean 3-space.Your axioms should also have the property that the words “point” and “plane” can beinterchanged while the word “line” stays the same.

3. In the definition of being in perspective with respect to a point we note that corre-sponding points must be distinct. What happens if they are not distinct? Is Desargues’Theorem still true? What happens if corresponding lines are not distinct?

4. In the Fano projective plane of order 2, does Desargues’ Theorem hold? Try a fewcases. But be careful to allow yourself to consider cases when some of the six pointsof the two triangles coincide. Some coincidences are forbidden by the hypothesis ofDesargues’ Theorem and some are not.

5. The notion of two triangles being in perspective with respect to a point depends onthe correspondence between the points of the two triangles. Can two triangles be inperspective with respect to different correspondences?

6. (Tricky) It was noticed that there was a duality in 3-space where “points” and “planes”are interchanged. In the proof of Desargues’ Theorem the notion of two (point) trianglesin 3-space being in perspective with respect to a point was generalized from the plane.A triple of planes can be viewed as a polyhedral “corner”. Draw a picture of this andshow how the statement of Desargues’ Theorem holds in this context.

7. In Chapter 2 we discussed projection from a point as a function from the points incidentto one line to the points incident to another line. What is the analogous function for theprojection from a line in the plane? What about projection from a plane in 3-space?

8. It was mentioned that projections are one-to-one and onto. Where do points above thehorizon in the picture plane come from (under f) in the object plane? (Use the formaldefinition of f . Our artist has an eye in the back of his head.)

9. In the following Figures 3.15 and 3.16 there are two shaded triangles. In each caserecord the center of perspectivity and the correspondence between the vertices of thetwo triangles. Then describe the line of perspectivity for the two pairs of triangles.Each line can be described by two distinct points that are incident to it, and any pointcan be described by the letter in the figure or by two lines that are incident to it. Forexample, the triangle ABC is one of the pair of triangles that are in perspective in bothfigures.

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10CHAPTER 3. SOLID GEOMETRYANDDESARGUES’ THEOREMMATH 4520, FALL 2017

EF

B

CA

GD

Figure 3.15

EF

G

AC

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D

Figure 3.16

10. In Figure 3.17 use Desargues’ Theorem to show that if the lines 64 and 152 are parallel,and the lines 45 and 163 are parallel, then the lines 56 and 243 are parallel.

11. In Figure 3.18 the quadrilateral on the left is a parallelogram with opposite sides par-allel. The line 57 is parallel to the lines 16 and 24.

(a) Show that the line segments 15 and 52 are of the same length.

(b) If an artist draws a picture of the figure on the left she gets something like thefigure on the right, where the three parallel lines 16, 24, and 57 that were incidentto a point at infinity, then become incident to a finite point 3′ as in the figure onthe right. 1′6′ and 2′4′ remain parallel. Show that 1′5′ and 5′2′ are of the samelength.

(c) Use the results above to show that Figure 3.17 can only occur if 7 is the centroidof the triangle 123 and 4, 5, 6 are the centers of their respective sides.

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3.2. EXERCISES: 11

6

7

5

4

1 2

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Figure 3.17

4'

5'5

7

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1 2

6

2'1'

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6'

Figure 3.18