Consider a large iron grate (G) in the shape of a right triangle, as shown in the figure below, The grate has to move from its current position to cover the hole (H). It must fit exactly within the dotted lines.
The grate is far too heavy to be lifted by hand, so a machine has been rigged that can lift the grate and flip it around any desired axis, thereby placing it on the other side of the turning axis. The action of the machine is shown in the figure below. If necessary, the axis can pass through the grate.
Find a sequence of flips that will move the grate to cover the hole. What is the minimum number of flips it will take to cover the hole?
The machine is a “reflecting” device—after the machine does its work, the new position of the grate is the reflection through the axis of the original position of the grate. The solution to the problem is that the grate can be moved in a step-by-step manner to cover the hole in three flips, and the minimum number of flips necessary is three. A sequence of flips is depicted in the figure below.
The first step uses a reflection through the line l, which is the right bisector of the segment joining the right angle vertex B of the grate with the corresponding vertex of the hole. With this reflection, the grate ABC is moved into position A′B′C′.
We now have one vertex in the correct position. Vertices A′ and C′ are not in the correct position, and the next step is to do another flip to get one of them into the correct place.
In (2), vertex C″ of the hole corresponds to vertex C′ of the moved grate, and by relecting A′B′C′ about the right bisector of C′C″ we can move C to the correct positon.
Note that the right bisector of C′C″ passes through B′ because B′C′ = B′C″. After the second step, the grate is in position A″B′C″. The third and final step is to reflect A″B′C″ about the line B′C″.
Earlier we defined the composition of two isometries. This terminology is used for any collection of transformations. If T and S are two transformations, the composition or product of T and S is denoted by either S T or ST. In terms of the individual points in the plane, ST acts as follows. First, the point X is mapped by T to T(X), then T(X) is mapped by S to S (T(X)). In other words, for each point X in the plane:
To move the grate to its desired position, we applied the product Rn Rm Rl of three reflections. Again, we emphasize that we follow the “right-to-left” rule. When evaluating Rn Rm Rl(X), first find Rl(X), then Rm (Rl(X)), and finally Rn (Rm (Rl (X))).
In the iron grate problem, we used the product of three reflections to shift the grate to its desired position. If we had a better machine—one that could perform rotations as well as reflections—we could accomplish the same thing by performing just two operations, as shown in the figure below.
In this case, the grate is moved by applying the product Rs RO,α. In the first solution, we used Rn Rm Rl. The individual transformations that make up the two products are quite different, but the net effect is the same. So we can write:
Two transformations are said to be equal if they have the same effect on every point in the plane. In other words, saying that T = S means that T(X) = S(X) for every point X in the plane.
As the example shows, T = Rs RO,α and S = Rn Rm Rl does not mean that T and S necessarily have the same description. The situation is similar to equality of functions in trigonometry: if
then the functions f and g are equal (since we have pointwise equality), although their descriptions are quite different.
Other examples of equal transformations that are defined differently are the halfturn and a reflection in a point.
The halfturn about a point O, denoted by HO, is the transformation RO, 180°. The reflection in the point O is the transformation that takes each point P to the point P′ so that O is the midpoint of PP′. The point O is called the center of the halfturn or the center of reflection. In the plane, since a reflection through a point is identical to a halfturn, there is no further need to talk about reflections through a point, and there is really no need for a special symbol to denote it.
In Chapter 7, we mentioned that the composition of two isometries results in a transformation that is also an isometry. In algebra, we would describe the situation by saying that the set of isometries of the plane is closed under the operation of composition.
More generally, if is a set of elements and if is a binary operation on , we say that is closed under the operation if for every pair of elements a and b in the product a b is also in . For example, the set of positive integers is closed under addition.
If R, S, and T are three transformations, the product TSR means first apply R, then S, and then T. For a point X, the notation TSR(X) means T (S (R(X))).
We can overrule this by using parentheses since the operations inside parentheses are carried out first. The notation (TS) R is interpreted as follows: first, determine what (TS) is. It will be some transformation, call it H, and H is usually different than either T or S. The notation (TS) R means HR; that is, first apply the transformation R, then apply the transformation H.
For example, let us suppose that S and T are reflections about two different parallel Lines and R is a rotation. Then, as we will see later, TS is some translation H. So we interpret (TS) R as meaning first do the rotation R, then follow it by the translation H.
In a similar way, the notation T (SR) means that we should first determine what SR is, namely, some different isometry L, and then take the product of L and T: T (SR) = TL. Note, however, that the parentheses in this case could be omitted, because in the absence of parentheses, the expression is evaluated from right to left.
The following theorem shows that (TS) R and T (SR) are equal.
Theorem 8.1.1. (Associative Law)
The associative law holds for the product of transformations; that is, given three transformations T, S, and R in the plane,
Proof. Let X be a point in the plane. We will evaluate T (SR) (X) and (TS) R(X).
The notation T (SR) (X) means “first evaluate SR(X), then evaluate T (SR(X)).” By definition, SR(X) = S (R(X)), so
The notation (TS) R(X) tells us to evaluate TS (R(X)). Now, TS(Z) = T (S(Z)) for all Z in the plane. In particular, when Z = R(X), we get
Thus,
Since (TS) R and T (SR) have the same effect on every point X in the plane, we conclude that they are equal transformations.
In algebra, a set of elements together with a binary operation · is called a group and is denoted by (, ·) if it possesses the following properties:
If it is also true that the commutative law holds (that is, if a · b = b · a for all a and b in ), then is called an Abelian group.
The notation for the binary operation · is usually omitted, so that we write ab instead of a · b.
We learned in Chapter 7 that every isometry has an inverse. This, along with the results of the previous section, show that the family of isometries in the plane, together with the composition operation, satisfy all four of the conditions listed above. We can summarize this with the following theorem:
Theorem 8.2.1. The set of all isometries of the plane, together with the operation of composition, forms a group.
Given an isometry T, we denote its inverse by T−1. Theorem 7.2.1 stated that
Example 8.2.2. What are the inverses of Gl, AB and HO?
Solution. We have
In any group, an element a other than the identity e such that a2 = a · a = e is called an involution. In other words, an involution is an element other than the identity that is its own inverse.
Any transformation that is an involution in a group of transformations is said to be an involutory or involutoric transformation; that is, T is involutory if and only if TT = T T = I. Among the transformations
the involutions are Rl, HP, and RP, θ when θ is a multiple of 180°.
In the figure above, triangle ABC has been carried into A′B′C′ by a reflection in the line m. The orientation of the triangle has changed—the path ABC proceeds in a clockwise (or negative) direction around the triangle, while the image path A′B′C′ goes in a counterclockwise (or positive) direction. This reversal of orientation will obviously happen to every triangle to which Rm is applied, and Rm is therefore called an opposite isometry. In general, any isometry T that reverses the orientation of every triangle is called an opposite isometry. On the other hand, an isometry T that preserves the orientation of every triangle is said to be a direct isometry.
There is a strong analogy between the products of direct and opposite isometries and the products of positive and negative numbers: direct isometries are like positive numbers and opposite isometries are like negative numbers. Some people prefer to draw an analogy to the addition of even and odd numbers, with direct isometries corresponding to the even numbers, so that the product of a direct and opposite isometry is like the sum of an even and an odd number. Some texts use the terms even and odd isometries instead of direct and opposite isometries.
Theorem 8.2.3. The product of two direct isometries is a direct isometry. The product of two opposite isometries is a direct isometry. The product of a direct isometry and an opposite isometry is an opposite isometry.
Theorem 8.2.4. The direct isometries of the plane form a group .
Proof. It is clear that is closed (under multiplication). Since the associative law holds for all transformations, it also holds for . The identity map is a direct isometry; that is, I is in . Every isometry has an inverse, and an isometry and its inverse are either both direct or both indirect. Therefore, whenever T is in , so is T−1. This completes the proof.
It is relatively easy to invent a transformation of the plane that is neither direct nor opposite. For example, let B and C be two different points in the plane, and let T be the transformation that interchanges B and C but leaves every other point where it is. The transformation T is almost the identity map, and there are many triangles PQR that remain unchanged under T. However, if A is a point that forms a triangle with B and C, the transformation maps A, B, and C to A, C, and B, respectively, thereby reversing the orientation. In other words, T preserves the orientation of some triangles while reversing the orientation of others. Thus, T is neither direct nor opposite.
The situation where T is an isometry is quite different as a consequence of two fundamental theorems about isometries in the plane, namely, that a plane isometry is completely determined by its action on three noncollinear points and that every plane isometry is the product of at most three reflections.
We begin the proofs of these facts with a theorem that characterizes the identity transformation.
Theorem 8.2.5. If T is an isometry that fixes each of three noncollinear points, then T is the identity.
Proof. Let A, B, and C be three collinear points that are fixed by T, so that
We want to show that T(X) = X for every point X in the plane. Suppose that this is not the case. Then there is a point P such that
Since T is an isometry with T(A) = A and T(P) = P′, we have
This means that A is on the right bisector of PP′. Similarly, B and C must also be on the right bisector of PP′, contradicting the fact that A, B, and C are noncollinear. This contradiction shows that our supposition that T is not the identity must be false and completes the proof.
When we say that a transformation T fixes a point X we mean that T(X) = X, and the point X is called a fixed point of T. In Martin’s text [50], he uses the phrase “T fixes a set ” to mean that under T the image of is . He uses the phrase “Tfixes S pointwise” to means that T(X) = X for each point X of . Another way of saying the same thing is to say that the set is invariant under the transformation T.
As an example of the difference in the meaning of this language, consider the mapping of an equilateral triangle ABC onto itself by a rotation of 120° around the centroid. The triangle ABC is fixed by the transformation, but it is not fixed pointwise.
Question 8.2.6. Suppose that an isometry fixes each of two different points. Can we assume that the isometry is the identity?
One of the virtues of group theory is that once you have proven a theorem about groups, it is valid for every group and does not have to be proven separately for each different group. Here is a very simple yet useful result:
Theorem 8.2.7. Let a and b be elements of a group (, ·) such that a · b = e, where e is the identity. Then a = b−1 and b = a−1.
Proof. Since G is a group, the element a has an inverse a−1. Multiplying each side of the equation
by a−1 on the left, we have
so that
and so
and thus, b = a−1.
The proof that a = b −1 can be obtained by multiplying the equation a · b = e on the right by b−1.
The following theorem can be proven in much the same way as Theorem 8.2.5, but we can give a more satisfying proof by using the fact that the isometries of the plane form a group. This proof illustrates how nicely algebra fits with geometry.
Theorem 8.2.8. An isometry of the plane is completely determined by its action on three noncollinear points.
Proof. Let A, B, and C be three noncollinear points in the plane, and let S and T be two isometries such that
We want to show that S = T. Now, since the isometries of the plane form a group, we know that T has an inverse T−1 so that
Thus, the isometry T−1S fixes each of the points A, B, and C, and by Theorem 8.2.5, this means that T−1,S must be the identity. By the previous theorem, S must be equal to the inverse of T−1; that is,
Theorem 8.2.9. Every isometry of the plane that is not the identity can be decomposed into the product of at most three reflections.
Proof. Let T be a given isometry, and let A, B, and C be three noncollinear points.
From the iron grate example, we know how to map A, B, and C to T(A), T(B), and T(C), respectively, by a sequence of at most three reflections.
Suppose that it actually took three reflections, say,
in that order. Then
Thus, Rn Rm Rl and T both have exactly the same effect on A, B, and C, so Rn Rm Rl = T, by Theorem 8.2.8.
Theorem 8.2.9, together with the fact that a reflection in a line is an opposite isometry, now allows us to show that every isometry in the plane is either a direct isometry or an opposite isometry.
Theorem 8.2.10. Every isometry in the plane is either a direct isometry or an opposite isometry.
Proof. If the isometry T is the identity or the product of two reflections, it is a direct isometry. If T is a reflection or the product of three reflections, it is an opposite isometry.
In this section, we use reflections to show that there are only four different types of plane isometries: reflections (in a line), rotations, translations, and glide reflections. We begin by examining the product of two reflections.
Example 8.3.1. Let l and m be two distinct parallel lines. Show that RmRl = TXY, where is a directed segment perpendicular to l and m and twice the distance from l to m.
Solution. Let h be a line parallel to l and m such that l is midway between h and m, as in the figure above.
Let A and B be points on h and let C be a point on l Rl maps A and B to points A′ and B′ on m and leaves C where it is.
Note that the two directed segments and are parallel and twice the distance from l to m.
The reflection Rm leaves A′ and B′ where they are and maps C to C′, where is parallel to and equal in length and direction to .
Thus, the effect of Rm Rl is to map A, B, and C to A′, B′, and C′, respectively.
However, the translation TAA′ also does the same thing, and by Theorem 8.2.8,
which completes the proof.
Example 8.3.2. Let l and m be two different lines intersecting at a point P. Show that Rm Rl = RP,θ, where θ is twice the directed angle α from l to m.
Solution. Let h be the line through such that the directed angle from h to l is α, and let n be the line through such that the directed angle from m to n is α, as in the figure above.
Let A be a point on h and let C be a point on l. Note that A, C, and P cannot be collinear. If they were collinear, then h = l, and it would follow that l, h, and m are all the same line, which is a contradiction.
Consider the effect of Rm Rl on the points A, P, and C. It is clear that RP,θ has exactly the same effect, so by Theorem 8.2.8, Rm Rl = RP, θ.
If l and m are the same line, then Rm Rl is the identity. This fact, together with the previous two examples, proves the following theorem:
Theorem 8.3.3. The only direct isometries of the plane are the identity, the translations, and the rotations.
We next turn our attention to the product of three reflections.
Theorem 8.3.4. Let l, m, and n be three lines with a common point P. Then Rn Rm Rl is a reflection.
Proof. If l and m coincide, then
If n and m coincide, then
If neither of these two cases occurs, we proceed as follows: let α be the directed angle from l to m. Now, there is a unique line h through P such that the angle from h to n is α
Thus,
and, therefore,
To handle the combination Rn Rm Rl when the lines l, m, and n are all different and have no point in common, we break it down into separate cases. First, we consider the cases where l and m are both perpendicular to n, then the cases where m and n are both perpendicular to l.
We note first that if all three lines are parallel, then Rn Rm Rl is a reflection. We leave the proof of this as an exercise.
Theorem 8.3.5. Let l, m, and n be three different lines.
Proof. For (1), we have Rm Rl = TAB by Example 8.3.1, and so Rnn Rm Rl is the glide reflection Rn TAB = Gn, AB as claimed.
For (2), Let A = l ∩ m, let B = l ∩ n, and let C be any point on m other than A. We leave it as an exercise to show that
for each of the points X = A, B, C so that
by the fundamental Theorem 8.2.8, and Rl Rn Rm is the glide reflection Gl, CD by (1).
The cases not covered by the previous theorem are depicted in the figures below, which show the possible arrangements of the reflecting lines.
Although arrangements (1), (2), and (3) appear to be identical, they are not the same because the order of the reflections matters. It may appear that these cases are complicated, but the associative law comes to the rescue in a rather magnificent way.
Theorem 8.3.6. Let l, m, and n be three nonconcurrent lines. Then Rn Rm Rl is a glide reflection.
Proof. The proof of each of the four cases is very similar. Here is how it is done for case (4).
The combination Rm Rl is a rotation about A through the angle 2α, where α is the directed angle from l to m, as in (1) below. Let m′ be a line through A perpendicular to n, intersecting n at C′. Let l′ be the line through A such that the angle from l′ to m′ is α, as in (2) below. Then
Now apply the associative law:
The transformation Rn Rm′ is the rotation HC′ Let n″ be the line through C′ perpendicular to l′, and let m″ be the line through C′ perpendicular to n″, as in (3) below. Then
Therefore,
and since m″ and l′ are parallel and both perpendicular to n″, we have a glide reflection.