A Beginner's History of Philosophy, Vol. 2: Modern PhilosophyCushman, Herbert Ernest
Philosophy
A Beginner's History of Philosophy, Vol. 2: Modern Philosophy
Cushman, Herbert Ernest
Philosophy -- History
Herbart agreed with Kant that we can experience only phenomena. There
is also a similarity in the two theories as to the relationship between
phenomena and the thing-in-itself. The similarity is, however, only
superficial. Kant reasoned from the relativity of phenomena to the
synthetic unity of apperception, _i. e._ to consciousness in general,
while the ♦thing-in-itself was to Kant an unknowable and irreducible
remainder. To Kant phenomena pointed to consciousness rather than
to things-in-themselves. On the other hand, Herbart reasoned from
phenomena to the existence of things-in-themselves. Phenomena point
to an independent, objective reality rather than to a thinking subject.
While in Kant’s doctrine phenomena depend for their existence upon
the creative power of consciousness, to Herbart consciousness has no
creative power, but itself depends on the existence and independence
of a plurality of independent Reals. Even the categories and the forms
of space and time are not innate synthetic forms. All are the result of
the relationships among independent Reals, which are the spring of all
activity and existence. Herbart thus gave to the things-in-themselves
all the independent functions that Kant attributed to consciousness.
=The Many Reals and Nature Phenomena.= We must remove the
contradictions of experience, if we would get at a true conception of
Reality and the meaning of phenomena. The true way is (1) to posit a
plural number of Reals, and (2) to interpret the phenomena as derived
from the relation among these Reals.
In the first place, a multiplicity of Reals, and not a single Real,
is needed to explain the multiplicity of phenomena. Herbart’s doctrine
is therefore a pluralism. He conceives the many Reals to exist, not in
phenomenal, but in “intellectual space.” They are not subject to any
phenomenal limitations whatsoever; they may occupy one point of space
at the same time. Their nature cannot be known, but we can say that
they have “absolute position.” They cannot be limited nor negated, and
even their plurality does not mean that they limit one another.
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