Entropy
Entropy is a measure of chaos. The second law of thermodynamics suggests
that our entire universe is slowing down, because its entropy, or its need for
sustaining energy, is increasing. One of the results of this law is the
prediction there that can be no perpetual motion machine (the first law tells us
no perpetual motion machines exist of the “first kind;” the second law of
the “second kind”). All systems wear down; energy is lost and cannot be
totally recovered by a system. We can also consider entropy to be a measure of
internal randomness, or molecular chaos. As entropy increases, chaos increases.
Arthur Eddington called entropy, time's
arrow and this name has been adopted by modern science (Angrist & Hepler,
1967). Entropy is an important concept in thermodynamics. The second law of
thermodynamics defines entropy as a measure of needed energy. Entropy is a
measure of a system's disorder. Entropy is also a measure of molecular
randomness. Thus a solid has less entropy than a liquid, which has less than a
gas (Angrist & Hepler, 1967).
The inequality of Clausius, a corollary of the second law, states that
any change in energy with respect to temperature must be less than, or equal to,
zero. In other words, the energy of any periodic system naturally tends to
decrease. Mathematically we can say that:
|
ŠdQ
/ T # 0 |
so
that entropy, S, over an entire cycle
of a system, can be defined for a reversible process as:
|
dS = dQ
/ T |
Here S is called the Clausius's
Entropy after Rudolph Clausius, who first conceived the idea of entropy.
For closed systems (systems that function independent of their
environment) it can be demonstrated
that:
|
dSsystem + dSsurroundings
$ 0 |
This equation expresses the
principle of the increase of entropy. All processes in closed or isolated
systems have increasing entropy. This is another way of saying that only those
processes can naturally take place where entropy will increase. This is a law of
closed-system thermodynamics. This law applies to all physical engines including
our bodies and to all systems including our world when they are considered
closed or isolated from their environments.
The general equation for an open system is:
|
dS $
dQ/T + dmisi - dmoso |
As a tiny mass dmi enters into the system, the entropy is increased by
the amount dmisi.
As the mass dmo leaves the
system, the entropy is decreased by the amount dmoso. In addition mass, energy, and
information can also be exchanged across the boundary of an open system. Until
recently, one spoke of systems as being either closed to their environments, or
open to them. Today, thermodynamics recognizes three types of systems: (1)
isolated, which do not share matter or energy with their environments, (2)
closed, which share energy and/or information but not matter, and (3) open,
which share matter and energy and/or information. (Kondepudi & Prigogine,
1998)
There are several other entropies today in addition to that of Clausius.
Prigogine's Entropy, for example, addresses what is called far-from equilibrium thermodynamics which looks at nonlinear dynamic
processes and self-organizing systems such as the cells of our body. The
equation for Prigogine's Entropy is:
|
dST = dSI
+ dSE |
where
dST is the total entropy
change, dSI is the change
in internal, or Clausius' Entropy, the entropy produced by irreversible internal
processes, and dSE is the
entropy exchanged with the surroundings (this term is zero for isolated systems
for which Prigogine’s Entropy is identical to Clausius’ Entropy). While dSI
tends to increase, the term dSE
can increase or decrease or remain zero (it is positive if entropy enters the
system and negative if entropy leaves the system). The important effect of
Prigogine's Entropy is that the total system, entropy change of any open system,
dST, can be positive, negative, or zero. Systems for which
dST < 0 (i.e.,
where entropy is decreasing) are said to be self-organizing
(Çambel, 1993).
Prigogine's Entropy implies that as systems become more complex, a
threshold of complexity will be reached such that the system will begin
functioning in unpredictable directions; such a system will lose its initial
conditions and these can never be reversed or recovered (Briggs & Peat,
1989). For open systems, where dSE is sufficiently negative that it
exceeds the magnitude of dSI, then
entropy will decrease (order will increase) over time during the process. This
could help explain the thermodynamics of dissipative systems (those that
required energy from external sources) and self-organizing systems (such as all
living systems) (Kondepudi & Prigogine, 1998; Nicolis & Prigogine,
1989).
Jacobi (1973) discusses entropy as:
Systems
accessible to our experience are only relatively self-contained, we nowhere
observe absolute psychological entropy, which could occur only in a perfectly
self-contained system. But the more the partial psychic systems are closed off
from one another and the more extreme the tensions between the poles, the more
likely becomes the phenomenon of entropy (cf. The stiff, catatonic posture of
many insane persons, their lack of contact with the world, their apathy, and
seeming lack of ego, etc.). We often see this law, in a relative form, at work
in the psyche....The irreversibility that characterizes energetic processes in
inanimate nature can be modified only by artificial intervention (e.g., by
technical or mechanical means). In the psychic system it is consciousness that
can intervene to bring about a reversal. (pp. 56-57)
Both Jung and Jacobi necessarily addressed the entropy of Clausius which
only holds for closed (i.e., isolated) systems (Prigogine’s Entropy for open
systems was not widely accepted until the 1980s). However, as Jacobi rightly
notes, the psyche is never totally closed to its environment. Although matter
does not cross into or out of the psychic boundary, both energy and information
do. Today, we would apply
Prigogine’s Entropy to the psyche as a self-regulating open system. The
terminology here may be confusing. The
psyche is open to both energy and information, but not to matter (which is but a
form of energy according to Einstein). In modern terminology, it would thus be
called a closed system, but we will denote it as open throughout the remainder
of this book to avoid confusion. The entropy of the psyche can be effectively
increased (leading to an equilibrium state such as the emptiness of ego
described by Jacobi above) or decreased (leading to normal healthy functioning)
through the interfaces with both its external and internal environments.
If we think of complex systems as being composed of millions of tiny
subsystems (for example, the cells in our body, the citizens of a country, or
the molecules in an object) then we will discover that each subsystem can act
randomly while the overall system itself is in equilibrium and is relatively
predictable. The theory of statistical
mechanics, invented at the end of the last century, is one way of dealing
with such subsystems. In this view, the system itself functions on the averages
or probabalistic actions of its
subsystems. For example, this is true for dissipative
structures that are also autopoietic or
self-organizing structures, which is to say, for living systems. Living systems
maintain their dissipative structure by dissipating entropy before it has a
chance to build up. Statistical entropy was created by the Austrian physicist,
Ludwig Boltzmann. His equation is usually given as
|
S
= -k E pi
loge pi |
where
S is the entropy, pi is the
probability of accessible states, and k is the Boltzmann Constant.
The higher the pi, the higher the entropy (Çambel, 1993). Boltzmann’s
Entropy indicates that entropy will always tend towards a state of maximum
probability (Lebowitz, 1993). In order to apply this equation, all of the
accessible states must have the same probability of occurring (Fast, 1962).
When we view entropy as a measure of chaos, we can say that the
probability of accessible states for any complex system is a measure of that
system’s uncertainty. Ludwig
Boltzmann was the first to note that entropy is a measure of molecular disorder
and he concluded that increasing entropy implied increasing disorder (Prigogine,
1980). Irreversible thermodynamics deals with systems that change over time, but
until recently it addressed only systems that are near to equilibrium conditions
(Angrist & Hepler, 1967; Prigogine, 1997; Kondepudi & Prigogine, 1998).
Jung wrote prior to the discovery of Prigogine’s Entropy. Thus, he was
persuaded to regard the psyche as a “relatively closed system” in order to
address the concept of entropy: He wrote:
According
to Boltzmann’s formulation, this leveling process corresponds to a transition
from an improbable to a probable state, whereby the possibility of further
change is increasingly limited. Psychologically, we can see this process at work
in the development of a lasting and relatively unchanging attitude.
(Jung, 1981, p. 26)
For Jung (1976), the psyche is governed by two important principles,
entropy and the principle of equivalence.
According to the principle of equivalence, any energy that disappears in one
area of the psyche must appear in another area.
Jung (1976) called the energy of the psyche the libido
and described it as coursing through the psyche rendering its contents either
conscious or unconscious. He writes, “We can say, then, that the concept of
libido in psychology has functionally the same significance as the concept of
energy in physics” (p. 131).
The principle of equivalence is similar to the law of the conservation of
energy found in physics. The total amount of libido remains constant but pockets
of it can ebb and flow at various places throughout the psyche. Jung viewed the
psyche as an arena where polar opposites are continually being balanced. Forces
at the higher end of the psyche, the spiritual side containing the archetypes,
are balanced by forces at the lower end of the psyche, the material side
containing the instincts:
The psyche is made up of processes whose energy springs from the equilibration of all kinds of opposites. The spirit/instinct antithesis is only one of the commonest formulations, but it has the advantage of reducing the greatest number of the most important and most complex psychic processes to a common denominator. So regarded, psychic processes seem to be balances of energy flowing between spirit and instinct. (Jung, 1981, p. 207)
When the psyche is considered as an open complex system, the law of energy conservation no longer applies. The psyche, like the physical body is dissipative, not conservative. Although Jung realized that the psyche is a complex dynamic system, it is now seen to be a great deal more complex than he believed. For example, while the libido is conserved, entropy can increase or decrease as the psyche interacts with its inner and outer environments--a fact unknown to Jung.