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Location: http://www.cs.mun.ca/~ulf/gloss/obj.html.
By Ulf Schünemann since 2002.
Please mail any comments.
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| navigation bar: Universals (properties, attributes, features, forms, types) | |||||
| object = universals (shared) + X (unshared) | concrete obj.: properties <-> concept: attributes | individual: properties <-> particular: features | properties <-> classes | ontological status of universals | attributes denote properties |
| unshared, ie. particular | shared, ie. universal | |||||||||||||||||||||||||||||||||
| I. Nominalism: | concrete object | = collection of things | (objects sharing 'things' means they overlap, not that 'things' are universals)| II. Bundle theory:
| concrete | object = bundle of
| properties | III. Substance theories | Bottom-up analyses: | A. Plato:
| concrete | object = formless matter
| + form | B. Smith:
| = patterned particularity
| + separation, stabilization, abstraction by observer | Top-down analyses: | C. Aristotle:
| concrete | object = primary substance |
| + properties | D. Bunge:
| = atomic bare individual(s)
| + bare associations | (=> aggregate bare individual) + properties | | ||||||||
Substance theory: An object is something over and above the properties that inhere in it [wiki]
Realm of Flowing Physical ParticularityIt contains particulars, not universals, and is presumptively not discrete [OOO] -> more |
Realm of Universals |
| concrete object = formless matter [physical] (what flows) + form [abstract] (how it flows) |
| concrete object/individual = physical particularity (fuzzily patterned) + separation & stabilization & abstraction |
Caveat: Smith here makes a non-standard distinction
between particularity and (material or abstract) individuals.
- Particularity and individuality are
«two overarching metaphysical characteristics ... that are essential
to our everyday conception of at least ordinary material objects.
Both ideas ... come together when we conceive of a stable and enduring thing,
such as a table, an old notebook, or a favorite bristelcone pine. ...
It is helpful to separate them, however, not only because they have different
conceptual structures, but also because ... they stem from different sources.»
[OOO 117]
«The whole point is «to separate the sense of the very specific or local
or "peculiar," to be associated with particularity, from the quite different
sense of being discrete or chopped up into distinct units or wholes, to be
associated with individuality» [OOO 120].
«[P]articularity and individuality, as I am using the terms, are
conceptually orthogonal. This can be seen by observing that they occur
differentially, or at least potentially occur differentially»
[OOO 124].
«It is non-standard to distinguish particularity and individuality
... The traditional treatment is ...:
particulars are viewed as a kind of individual ...
Non-particulars, however - like generics, for example, and/or abstract entities
- are (or at least can be) counted as individuals, but not as particulars ...
Thus [the tiger] that snarled at your Land Rover yesterday,
would be a (bare) particular ... The type tiger, being abstract, would still
be individual, but ... not a particular ... The same would be true of the
generic tiger, the tiger that is threatened with extinction.
It is traditional, in other words, to take the word `individual'
to be essentially synonymous with `object' or `entity' - i.e., as denoting
the most general class, of which particular are taken to be an important,
or even the paradigmatic, species.» [OOO 123f]
- Particular.
«By `particular' ... I mean something like `occurrent': something that
is located or that happens, something that is embodied ... If one is a physicalist
... a possible alternative for `particular' might be `concrete.'
[OOO 117ff]
- Individual.
«By individuality ...
I mean whatever it is about an entity that supports the notion of individuation
criteria - something that makes `object' a count noun, something that makes
objects discrete. Somehow or other, an individual object is taken to be something
of coherent unity, separated out from a background ...
Etymologically, individual means indivisible: not to be divided.
That should not be taken as implying that individuals cannot be chopped up
at all ... Rather, it is to imply that, qua individuals, they have
an overall integrity or unity that is liable to be violated by taken them
apart. Because they are discrete, in other words, individuals support the
notion of half, as well as of two. Unlike water, if you put individual and
individual together, you get two individuals, not just more. By the same
token, if you taken an individual apart, you get parts or fragments, not just
less.« [OOO 119f]
- Individual vs identity:
«Because objects (individuals) play such a central ontological role ...
questions of identity are often assumed, by default, to be questions about
the identity of an individual. ... In practice, however, it is easy
to see that it is not always justified. Diffusions (such as fog), abstractions
(such as melancholy), and collectives (such as of people) can have
identities without necessarily being individuals,
or supporting individuation criteria.» [OOO 132]
«Identity ... is simply the property of being the individual
in question; it is not a feature or property relevant to whether
it is the indivudal in question.»
|
navigation bar: Universals (properties, attributes, features, forms, types) |
| object = universals (shared) + X (unshared) |
| concrete obj.: properties <-> concept: attributes |
| individual: properties <-> particular: features |
| properties <-> classes |
| ontological status of universals |
| attributes denote properties |
The Other RealmBut the physicist must have access to both realms. «Physicists must have some kind of physical or effective access to the [realm of particularity] in order to conduct their experiments ... This necessary involvement in the physical situation is what raises such perplexing questions in both relativity theory and quantum mechanics (e.g., about the collapse of the wave functions). On the other hand, it is equally necessary for physicists to have at least semantic access to the [realm of universals] in order to publish papers discussing or representing or stating those laws» [OOO 157]. |
| Statement = Term + Predicate |
| Cf. universality of logic and | ontological committment |
a) Hence, in terms of a compositional semantics of statements, there must not only be things (objects) denoted by the subject and argument expressions in the statement, but there must also be something meant by the predicate in the statement. For instance, in case of the statement "the apple is red" there must be some "apple" and something like the "red-being" or "redness".
b) Psychologically, in order to use and reason about such a statement,
one must know a referential concept "apple"
and a predicable concept "red-being".
«Referential and predicable concepts are not the same, but rather are
complementary, types of cognitive structures ...
That is, predicable concepts, as unsaturated cognitive structures based
upon capacities to identify, characterize, and relate objects in various
ways, are complemented in speech acts by referential concepts as cognitive
structures that enable us to refer (or purport to refer) to the objects
that we characterize and relate to one another. And, just as it is the
exercise of a predicable concept that informs such an act with a predicable
nature, so it is the exercise of a referential concept that informs that act
with a referential nature» [KRCR].
«Referential concepts are initially developed not in terms of reference to
objects in general but to objects of a sort--where, by a sort (or
sortal concept) [^],
I mean a type of concept (such as Raven, dog,
horse, car, tomato, etc.) whose use in thought and communication is
associatated with certain identity criteria, i.e. criteria by which we are
able to distinguish and count objects of the sort in question» [KRCR]
-> [IC].
|
Properties and property-spaces «The properties an object may have fall into natural groups or spaces of contraries. ... Provided we speak only of fully exact properties, in each of those spaces no object can simulataneously have more than one property-- it cannot have two masses, temperatures, etc. ... Such spaces of properties are often known by their own names, like `mass', `volume', and so on ... Following Johnson, we call mass, volume and the like determinables and the precise properties making up such a space determinates. So for the determinable mass there are indefinitely many determinates, including 1gm, 2gm, 3.78gm, and so on, and similarly for other determinables. Determinables are sometimes called `attributes' and their determinates `values' of these attributes. ... There are also multi-placed determinates, like distance (always of one thing to another) and angle (of one thing to another with respect to a third). By plugging gaps in multi-placed determinables we get determinables of fewer places, e.g., distance from Rome.» [Parts 343f] Property-space ("general property") P represented by propositional function S->P «A substantial property must ... be representable as a propositional function, or predicate, on a domain that somehow includes S [the set of substantial individuals]. The function will represent the property in general, e.g. age; and its value for a particular individual, the given property of the individual concerned, eg. its age. ... For example, mass is representable by a certain real valued function M on the set of quadruples <body, reference frame, time, mass unit>» [MB3 63]. |
| Object [referenced by term]
= mutable properties [predicated]
+ substance [basis of identification]
|
|
«[O]ur conceptual reconstruction of the notion of a real thing» [MB3 57]:
1. bare individual + bare association 2. property |
Bare individuals and non-individual properties are fictions:
«entities
deprived of most of their properties [except for their association],
forms without a definite stuff. However, we warned that these are fictions
and anticipated that they would enable us to construct
the notion of a real thing as a fully qualitied individual.
This is indeed what a concrete or material object,
such as a radio wave or a person or a society is:
namely an entity endowed with all its properties,
both intrinsic and mutual, permanent and transient» [MB3 110]
«The set of (unarized dichotomic) properties of individual
xT is called
p(x) = {PP | x possesses P}» [MB3 72].
«Definition 3.1 ... The individual together with its properties is called the thing (or concrete object) X» [MB3 111].
A formal object model based on this definition comes next
If "x's properties"
for a substantial individual xS
is formalized
as the set p(x)
P
of properties,
and if "A together with B" is formalized
as the tuple <A,B>
then concrete object X can be formalized as <x,p(x)>.
But note that «X =df <x,p(x)> ... characterizes a concept of a thing rather than being the "real definition" of a thing» [MB3 112]. <x,p(x)> is a formal model of concrete object X, not X itself: a concrete object is not a tuple (ie. a mathematical, not concrete, concept), nor does it comprise a set (which is another mathematical, not concrete, concept).
Functional schema «Theoretical science and ontology handle not concrete things but concepts of such, in particular conceptual schemata sometimes called model things. Our construal of a thing as a substantial individual together with the set of its properties ... is of course such a model thing - albeit a rather poor one. A richer characterization of a thing is given by a set equipped with specified relations, such as functions or operations. For example, if the thing represented is a force field, then the set will be a portion of a geometrical manifold M - e.g. a region in Euclidean three space - together with a tensor field F on M. Briefly, <M,F> ^= field» [MB3 119, underlining added]. «We shall adopt this mode of representation by making
Definition 3.6 Let X = <x,p(x)>
be a thing of class TThing.
A functional schema Xm of X
is a certain nonempty set M together with a finite sequence
F of nonpropositional functions on M,
each of which represents a [general] property of T's. Briefly,
«The base set M will be denumarable or nondenumerable,
as the case may be.
It may or may not be thought of as mapped on a subset of physical spacetime.
...
The finiteness of the set of components of F agrees with the part
of Postulate 2.3 specifying that there are finitely many
general properties [aka. property spaces, cf.]
(such as length or longevity). And it does not contradict the second part
of that postulate, according to which p(x) is nondenumerable
for each xS. Indeed, ...
a single continuous general property, such as age, gives rise to infinitely many
individual properties (such as successive ages) as the property in question takes values.
...
Example 1 The simplest functional model of a corpuscle with variable mass
is the classical mass point. Here M=F×T,
where F is the set of referenceframes and T=R the real line,
everypoint of which is interpreted as an instant of time.
And F=<mu,pi,psi> is a triple of functions on M=F×T,
such that mu(f,t) represents the mass,
pi(f,t) the position, and psi(f,t) the force acting on the corpuscle,
relative to frame fF, at time t
T» [MB3 120].
State functions
«The components Fi of the list F of functions
in a functional schema are usually called state variables
[or state functions]
because their values contribute to characterizing or identifying
the states the thing of interest is in» [MB3 125].
The Fi: M->Vi
have unspecified co-domains.
They represent the property spaces of X ("general properties").
Each value of Fi at a point mM
represents an ("individual") property of X.
F is called the total state function for X, and its value
F(m) = <F1,F2,...,Fn>(m)
= <F1(m),F2(m),...,Fn(m)>
for mM represents the state of X at m
in the representation Xm [MB3 127].
«Notice the cautious expression `in the representation Xm'. The reason is that there is no such thing as the absolute statefunction for a given thing: indeed there are as many state functions as functional schemata of the thing can be conceived» [MB3 127]. «The various functional schemata of a given thing need not be equivalent: for example they may exhibit different amounts of structure» [MB3 121]. «It goes without saying that things belonging to the same natural kinds - e.g. electrons, neurons, peasant societies- are represented by the same functional schemata. In particular, indiscernables are representable by the same model things. In other words, for theoretical purposes we may treat indiscernibles as if they were identifical - which of course they are not» [MB3 122].
For systems: «The domain A of the state function F os systems of kind K is the cartesian product of certain sets, such as K, the family 2E of sets of environmental items with which the members of K are coupled, the set F of reference frames, the set T of time instances, and so on» [MB4 20].
State space «Every theoretical model of a thing is concerned with representing the really possible (i.e. lawful) states, and perhaps also the really possible (lawful) changes of state, of the thing» [MB3 131]. «If we form the cartesian product of the codomains of the various components of F ... we obtain the codomain V of F itself, a set that will be called the conceivable state space for the thing represented ... However, a state function may not take values in its entire codomain but may be restricted to a subset of the latter, by virtue of some law ... In other words, because the laws impose restrictions upon the state functions and their values, hence upon the state spaces, only certain subsets of the latter are accessible to the thing represented. We shall call the accessible part of the state space the lawful state space of the thing in the given representation and relative to a given frame» [MB3 133]. «[F]ar from being something out there, like physical space, a state space for a thing [in the representation Xm] stands with one leg on the thing, another on a reference frame, and a third on the theoretician (modeller)» [MB3 132]. («While in most of general system theory the state space is assumed to be finite dimensional, the state (or Hilber) spaces occurring in the quantum theories are infinite dimensional. Every point in such spaces can be analyzed into infinitely many components, namely those along the axes constituted by the orthonormal eigenfunctions of an arbitrary hermitian operator in the Hilbert space» [MB3 136].)
«Any restriction of the posssible values of the components of F
and any relation among two or more such components is called
a law statement
iff (i) is belongs in a consistent theory about the X's and
(ii) it has been confirmed empirically to a satisfactory degree» [MB3 129].
«If a law statement concerns a certain thing x, we call it L(x),
and we may call L(x) = p(x)L
the totality of laws, or rather law statments, for x.
...
This is not a mere matter of notation for ... laws are properties.
And, being properties, they are representable as functions,
Indeed, a law statement may be construed as the value of a certain function
- a law function - with domain the class T of things concerned,
and codomain the set of law statements of the form L(x). In short,
The lawful state space SL(X) of thing X in representation Xm is
«If during the existence of a thing (e.g.
when it is being observed),
only some components of its state function change their values,
one says that the remaining components are ignorable
and the study of the thing can be restricted to the state subspace
spanned by the active state variables.
This subspace may be called the reduced state space» [MB3 136].
«Every state is a state of some concrete object or other:
there are no states in themselves. And conceptual objects are in no states whatsoever.
Therefore a thing could be defined as whatever is insome state or other.
Things differ by the states they are in, and their changes are changes of state.
But all the things of a given (natural) kind share the same (lawful) state space
- which is a way of saying that they share the same general properties.
In sum, states serve to characterize not only individual things
but also natural classes of things - hence the centrality of the state concept»
[MB3 139f].
Change
«Whatever changes may be thought of either as turning into a different thing
or as going into a different state. In the former case the change of interest
can be construed as the ordered couple <x,x'>, where x and x'
are the initial and the final things respectively. However, since names or
singular terms such as `x' and `x'' are not descriptive,
this representation of change is unilluminating. Nesides, it forces an
unnecessary multitude of the number of things. For this reason it is not
used in science and we shall not employ it in ontology.
«Every point s belonging to a lawful state space SL(x)
of a thing x represents a possible state of the thing.
The actual state of the thing is represented by what is called its
representative point in the state space.
An actual change of thing x is represented by a trajectory
of the representative point; this trajectory is of course the graph
of a certain function on SL(x).
It is convenient, through not indispensible, to express
the curve with the help of a parameter, the standard interpretation
of which is time. But one of the advantages of the state space representation
of change is that it requires no explicit use of the time concept» [MB3 216f].
«Definition 5.27 Let F be a state function for a thing x
relative to a reference f with states t in S(f),
and let the latter be coordinatized by a certain function
k: R4 -> S(f).
Then the history of x relative to f is the set of ordered pairs
«If there are considerable changes in the individual properties of a thing,
but the thing neither acquires nor loses any general property,
we may say that it undergoes a large change.
If on the other hand a thing gains or loses general properties
then it canbe said to undergo a deep change.
Whereas in the first case the axes of the state space remain fixed,
in the second some are added or removed.
We obtain a smooth description of this sort of change if we build
the state space will all the necessary axes and use at any given moment
only those portions of the total space that concern the properties
actually possessed by the thing at the moment» [MB3 219]
(cf. redunced state space).
Far more information is conveyed if the name `x' is replaced by
the sentence `thing x is in state s',
where s is a point (or a set of points) in a state space
S(x) for x. We can then construe a change of x
as a transition from state s to some other state
s'S(x).
In other words, we adopt what may be called the
principle of nominal invariance,
or permanence of names through change, and describe change as changes of state.
...
Principle 5.1 A thing, if named, shall keep its name throught its history
as long as the latter does not include changes in natural kind
- changes which call for changes of name.
... This allows us to designate a given person at age 50 by the same name
as at age 5 even though in between the person may have renewed every single
atom in his/her body. In short, there are no self-identical things
but only constant names helping us to keep track of the changes
undergone by things» [MB3 221].
S(f) }.
This is an elucidation of the concept of a life line, behavior line,
or trajectory. The history of a thing is regared as the succession of its
states but, instead of being represented by a line in the n-dimensional
state space spanned by F, it is represented as a curve in the
(n+4)-dimensional space R4×SL(x)»
[MB3 255].
«The thing undergoes a qualitative change iff
SL(x) equals the union of at least
two subspaces, eachof which is spanned by a different projection of F.
Otherwise (i.e. if none of the components can be ignored during
any stretch of the process), the thing undergoes only a
quantitative change.
Ulf Schünemann 120503