composite motion C with
9. Boolean Algebra
Another example of an algebra is provided by the operations such as the
intersection
and theunion
of subsets S andT
of a given set X. If we write X E S for "x is an element of S" and � for "if and only if', these operations are specified by giving the elements of the resulting subset of X as follows :9. Boolean Algebra
Intersection Union
X E S n
T
� X E S andx
ET,
X E S U
T
� X E S orx
ET,
27
( 1 )
(2)
=> X E S =>
T
� if X E S , thenx
ET,
(3)�
x
ET,
or not(x
E S) . They correspond exactly to the three propositional connectives "and","or", and "if then". They may also be pictured by Venn diagrams; if the set
X
is taken to be all the points in a rectangle while S andT
are respectively the points inside the ovals S and
T,
then two of these operations may be indicated by shaded areas as in Figure1 .
There is also a unary operation, thecomplement
.., S of S:x
E .., S � not(x
E S) (4)These various operations n, U, => , .., satisfy certain algebraic identities which can all be deduced from a suitable list of axioms, the axioms for
Boolean Algebra.
Thus the setP(X)
of all subsets ofX
is a Boolean algebra.
There also are operations on infinite families of sets. Thus if S; is a sub
set of
X
for eachi
in some "index" setI,
the (infinite) Union and intersection are defined by
x
E U S; � For somei
inI,
X E S; ,;
x
E n S; � For everyi
inI,
X E S;;
(5)
(6) These operations correspond to the logical quantifiers "There exists an
i"
and "For all
i",
respectively. These connections with logic will be explored further in Chapter XI.Boolean algebra provides a Mathematical way of representing proper
ties, in that each property H of elements of a set
X
determines a subset ofX;
namely, the subset S consisting of all those elements which have the propertyS =
{x I x
EX
andx
has H} .s
m
Ts n T S � T
Figure I . Boolean operations.
(7)
2
8
I . Origins of Formal Structu re This subset is sometimes called theextension
of the property H, to emphasize the notion that differently formulated properties may have the same extension-and that Mathematics has to do with extensions rather than with meanings. This in turn involves the "extensionality" axiom for sets-that a set is completely determined just by specifying its elements.This means that the equality of two subsets of
X
is described by the statement
S = T � (For all
x
inX,
X E S �x
En , (8)
while the inclusion of one subset S in another is described by
S c T � (For all
x
inX,
X E S �x
E n ; (9) here the arrow � stands for "implies".This inclusion relation is transitive, reflexive, and antisymmetric, as these properties were defined in §4 above. In general, an
ordered set W
is a setW
(such asP(X»
with a binary relation (such as S c T for S, T E W) which is transitive, reflexive, and antisymmetric. An ordered set is often said to bepartially
ordered (aposet)
because it need not satisfy the "trichotomy" property which holds for a linear order.It is important to recognize that many orders are just partial orders and not total orders (i.e.,
not
linear). However, in many domains of the application of Mathematics to social phenomena, there is a strong tendency to order ideas, people, and institutions in a
linear
way-for example, according to rank on some imagined numerical measure. The more relevant notion of partial order seems little known and less used.
Diagrammatic presentation of an inclusion relation is suggestive. Thus the various inclusions of the subsets of a three-element set can be pictured by the rising lines in Figure 2, where the bottom symbol 0 denotes the
empty
subset. The Boolean operations on subsets may be visualized in this figure. For example, the union { l ,2 } of the subsets { l } and { 2 } is the smallest subset which lies "above" both the subsets { l } and {2 } ; in this way it is the least upper bound, as defined in §4, of { l } and { 2 } . Generally, the union S U T of two subsets S and T of a set
X
has the properties
S c S u T, T C S U T, S c R and T c R � S U T c R ,
( 1 0) ( I I ) which state that i t i s the least upper bound o f S and T in the partial order given by inclusion. In an exactly dual way, the intersection S n T is the greatest lower bound of the subsets S and T. In other words, both these Boolean operations can be described directly in terms of inclusion,
1 0. Calculus, Continuity, and Topology
(1,2,3)
--- I �
(I ,
2} (1, 3}
(2'13}
---��
Figure 2. Lattice of subsets.
29
without any use of membership. In Chapter XI we will see further exam
ples of sets treated without the use of elements.
There are corresponding definitions for other inclusion relations. In general (and in view of diagrams like that above) a poset is said to be a
lattice
when it has a top elementI ,
a bottom element 0 and when each pair of elements have a least upper bound (called theirjoin)
and a greatest lower bound (called theirmeet).
The lattice of subobjects of an algebraic object is a way of describing some of the structure of that object.1 0. Calculus, Continuity, and Topology
Many notions besides those of transformation groups arise from the mathematical analysis of motion. The complex motions of the planets and the varying velocities of falling bodies suggest the idea of "rate of change" : Velocity as rate of change of distance or acceleration as rate of change of velocity. These ideas were codified in the notion of the deriva
tive, subsequently formalized (Chapter VI) in the rigorous foundation of the calculus, as based on the axioms for the real numbers. This uses the definition of the derivative by means of limits and thus the consideration of a class of "good" functions-those which are differentiable. As a first example of this circle of ideas, we examine here another good class-the functions which are continuous.
A rigid motion M:
F
-+F
of a figure is continuous because (by rigidity) the distance from Mp to Mq must equal that from p to q. For a function f: R -+ R on the real numbers R continuity means considerably less: Just thatfx
and fy will be close if the originalsx
and y are sufficiently close.This formulation is still pretty vague ; it should mean that one can make
fx
and fy "as close as you please" by requiringx
to be "suitably close"to y. This is still vague. "As close as you please" should mean "within a specified measure 8 (a positive real number) of closeness; "suitably close"
should mean that one can specify a measure of closeness (again a positive real number t:) which will do the job. All this (and we have telescoped a
30 I . Origins of Formal Structure
long and painful historical development) comes down to make the famil
iar (but meticulous) £ - 8 definition of continuity: A function
f:
R --> R iscontinuous
at a pointa
E R ifFor all real £ > 0 there is a real 8 > 0 such that, for all
x
in R ,( I )
If
I x
-a I
< 8 , thenI f(x ) - f(a) I
< (.
(2) If this statement holds forall
pointsa
E R, the functionf
is called continuous; the class of all such continuous functions is called
C.
Note that the statement involves both propositional connectives ("if . . . then") and the so called "bounded" quantifiers (For all real numbers, there exists a real number). Thus it is that careful formulations lead to the use of concepts of formal logic.
Topological and metric spaces arise from analysis of this definition of continuity. The inequalities used in the definition arise from ideas of approximation (approximations of the value b =
f(a )
to within the accuracy £ ) and so implicitly involve the open interval I. ( b ) =
{y I I y
- bI
< £ } of center b and "radius" £. In the familiar representation of the function
f
by itsgraph
(the set of points(x,
f(x » in the plane), this open interval appears as an open horizontal strip of width 2£around
y
=f(a )
(Figure 1 ). The definition is concerned with those pointsx
E R for which f(x ) lands in this interval I = I. (b )-this set of points is usually called theinverse image
of I under the functionf,
in symbols :f- II =
{x I x
E Rand f(x )
E I}.
Indeed, if Xo E
f
-II (that is, iff
(x
o) E I), then one can prove from the definition of continuity that there is an open interval (on thex
axis) of center Xo wholly contained in f - II. This amounts to theTheorem.
The function f:
R --> Ris continuous for all a
E Rif and only if the inverse image f
-I Iof every open interval of
Ris a union of open intervals.
- - - - - t
f(a) = b 2€
Figure I
1 0. Calculus, Continuity, and Topology 3 1
In other words, continuity can be described wholly in terms of open intervals.
Continuity is also needed for functions
f
defined on only a part of the real line, for functions of two or more variables, or for functions defined on a surface, etc. But this new definition requires no new ideas. The absolute valueI x - a I
which appears in the definition( I )
and (2) is just the distancep(x,a)
on the line R from the pointx
to the pointa.
Hence the same definition will work with any suitable notion of distance-that is, for a metric space.
Definition. If
X
and Y are metric spaces, a functionf: X
... Y is continuous at a point
a
EX
if for all real t: > 0 there is a real 8 > 0 such that for allx
inX,
ifp(x,a)
< 8 thenp(f(x),f(a»
< t:.In particular, this defines continuity for functions of two real numbers
x,y.
Just regard(x,y)
as the (coordinates of) a point in the plane R X R with the usual (pythagorean) metric P I =p,
p«x,y),(a,b »
=[(x - a i
+(y - b i ll/2 ,
Then in the definition of continuity the open interval consisting of all
x
with
I x - a I
< 8 is replaced by theopen disc
with center(a,b )
and radius 8. This disc consists of all points(x,y)
in the plane with(3) As in the theorem above, one can prove that a function
f:
R X R ... R of two real variables is continuous if and only if the inverse image of each open interval in R is a union of open discs in R X R.But the plane is also a metric space with a distance
P2
described as the"shortest path along the rectangular grid", so that
P2«x,y), (a,b»
=I x - a I
+I y - b I '
or with the distance given by
P3«X,y),
(a, b»
= Max(I x - a I , I y - b I ) .
For a function
f(x,y)
of two real variables, any one of these distance formulas may be used to define the continuity of
f
in the usual t: - 8 style.These different distances all yield the
same
continuous functions, so that continuity, viewed invariantly, depends not on distance but on something else more intrinsic. What is it? The answer is well-known. Each distance Ph f>2, or P3 will determine a series of "open circular discs" -circular in that metric-of the respective forms (interior of) circle, diamond, or square (Figure 2). Within each disc we can readily draw a smaller disc of the32 I. Origins of Formal Structure
Figure 2
other forms with the same center-so we get the same ( - 8 continuous function by just choosing different 8's to a given (.
What is the intrinsic formulation? In the alternative description of con
tinuity stated in the theorem above there appeared unions of open inter
vals and unions of discs. In any metric space
X
the opendisc
with centera
and radius 8 may be defined to be the set of all points x in
X
withp(x,
a
) < 8. Now define anopen set U
inX
to be any union (finite or infinite) of open discs. Equivalently, a subsetU
isopen
inX
if to each pointa
EU
there is a 8 > 0 such that p(x,a
) < 8 implies x EU
-every pointa
inU
is contained in an open disc centered ata
and withinU.
Now the continuity of f:X
... Y is expressed in terms of open sets: f is continuous if and only if the inverse image of any open set of Y is an open set ofX.
This is the desired intrinsic formulation, independent of the perhaps accidental choice of a metric. Specifically, the three different metrics p = P I , P 2 , and P3 described above for the plane all yield the same open sets, because any union of circular open discs is also a union of open squares or of open diamonds, and conversely. In this way, the notion of "open set" is more intrinsic than that of distance.This suggests that a space can be defined directly in terms of its open subsets. A
topological space
is a setX
in which certain of the subsetsU
are distinguished and called theopen
sets, and in which these open sets are required to satisfy the following three axioms :1 . The intersection of two open sets is open;
2. The union of any collection of open sets is open;
3.
X
itself and the empty subset 0 cX
are open.A
topology
on a setX
is then the specification of open subsets which satisfy these axioms. Thus any metricX
determines a topology, in which the open sets are the unions of discs open in the metric. There are also topologies not defined by way of a metric. For example, there is a topology on the set
N
of natural numbers for which the open subsets are the empty subset and all those subsets S with finite complement (inN).
There are many other examples of topologies.The definition of continuity (the inverse image of any open set is open) now applies to any function f:
X
... Y between topological spaces1 0. Calculus, Continuity, and Topology 33
Extensive experience has shown that this description of a "topology" in terms of open sets and neighborhoods is extraordinarily effective in for
mulating all sorts of Mathematical facts in a geometric form. The concept of "topology" has been appropriately abstracted from the many examples of "continuity".
The notion of a topological space was first presented by F. Hausdorff in a famous (and beautiful) book
Mengenlehre.
His definition was formulated differently, in terms of selected neighborhoods, and included an added axiom (the Hausdorff separation axiom): Two distinct points have disjoint neighborhoods. A topological space with this property is called a