A 'physical
paradox' is an apparent contradiction relating to
physical descriptions of the
universe. As such, there are many different uses for the term ranging from a challenging
thought experiment that seems to belie common sense to an actual breakdown of the
mathematical theory that describes the physical universe. While many physical paradoxes have accepted resolutions that make them little more than curiosities, others may defy resolution and be the result of an inadequate interpretation of the theory, an
assumption about the physical world that is violated, or an indication that the
theory inadequately describes the conditions. In
physics as in all of science,
contradictions and
paradoxes are generally assumed to be artifacts of error and incompleteness because
reality is assumed to be completely
consistent, although this is itself a philosophical assumption. When, as in fields such as
quantum physics and
relativity theory, existing assumptions about reality have been shown to break down, this has usually been dealt with by changing our understanding of reality to a new one which remains self-consistent in the presence of the new evidence.
Paradoxes relating to false assumptions
Certain physical paradoxes defy
common sense predictions about physical situations. In some cases, this is the result of
modern physics correctly describing the natural world in circumstances which are far outside of everyday experience. For example,
special relativity has traditionally yielded two common paradoxes: the
twins paradox and the
ladder paradox. Both of these paradoxes involve thought experiments which defy traditional
common sense assumptions about
time and
space. In particular, the effects of
time dilation and
length contraction are used in both of these paradoxes to create situations which seemingly contradict each other. It turns out that the fundamental
postulate of special relativity that the
speed of light is
invariant in all
frames of reference requires that concepts such as
simultaneity and
absolute time are not applicable when comparing radically different frames of reference.
Another paradox associated with relativity is
Supplee's paradox which seems to describe two
reference frames that are irreconcilable. In this case, the problem is assumed to be well-posed in special relativity, but because the effect is dependent on objects and fluids with mass, the effects of
general relativity need to be taken into account. Taking the correct assumptions, the resolution is actually a way of restating the
equivalence principle.
Babinet's paradox is that contrary to naive expectations, the amount of radiation removed from a beam in the
diffraction limit is proportional to twice the
cross-sectional area. This is because there are two separate processes which remove radiation from the beam in equal amounts:
absorption and
diffraction.
Similarly, there exists a set of physical paradoxes that directly rely on one or more assumptions that are incorrect. The
Gibbs paradox of
statistical mechanics yields an apparent contradiction when calculating the
entropy of mixing. If the assumption that the particles in an
ideal gas are indistinguishable is not appropriately taken into account, the calculated entropy is not an
extensive variable as it should be.
Olbers' paradox shows that an infinite universe with a uniform distribution of stars necessarily leads to a sky that is as bright as a star. The observed dark night sky can be alternatively resolvable by stating that one of the two assumptions is incorrect. This paradox was sometimes used to argue that a and
isotropic universe as required by the
cosmological principle was necessarily finite in extent, but it turns out that there are ways to relax the assumptions in other ways that admit alternative resolutions.
Mpemba paradox is that under certain conditions, hot water will freeze faster than cold water even though it must pass through the same temperature as the cold water during the freezing process. This is a seeming violation of
Newton's law of cooling but in reality it is due to
non-linear effects that influence the freezing process. The assumption that only the
temperature of the water will affect freezing is not correct.
Paradoxes relating to unphysical mathematical idealizations
A common paradox occurs with mathematical idealizations such as s which describe physical phenomena well at distant or global
scales but break down at the
point itself. These paradoxes are sometimes seen as relating to
Zeno's paradoxes which all deal with the physical manifestations of mathematical properties of
continuum,
infinitesimals, and
infinities often associated with
space and
time. For example, the
electric field associated with a
point charge is infinite at the location of the point charge. A consequence of this apparent paradox is that the electric field of a point-charge can only be described in a limiting sense by a carefully constructed
Dirac delta function. This mathematically inelegant but physically useful concept allows for the efficient calculation of the associated physical conditions while conveniently sidestepping the philosophical issue of what actually occurs at the infinitesimally-defined point: a question that physics is as of yet unable to answer. Fortunately, a consistent theory of
quantum electrodynamics developed in part by
Richard Feynman removes the need for infinitesimal point charges altogether.
A similar situation occurs in
general relativity with the
gravitational singularity associated with the
Schwarzschild solution that describes the
geometry of a
black hole. The
curvature of
spacetime at the singularity is infinite which is another way of stating that the theory does not describe the physical conditions at this point. It is hoped that the solution to this paradox will be found with a consistent theory of
quantum gravity, something which has thus far remained elusive. A consequence of this paradox is that the associated singularity that occurred at the supposed starting point of the universe (see
Big Bang) is not adequately described by physics. Before a theoretical extrapolation of a singularity can occur, quantum mechanical effects become important in an era known as the
Planck time. Without a consistent theory, there can be no meaningful statement about the physical conditions associated with the universe before this point.
Another paradox due to mathematical idealization is
D'Alembert's paradox of
fluid mechanics. When the
forces associated with
two-dimensional,
incompressible,
irrotational,
inviscid steady flow across a body are calculated, there is no
drag. This is in contradiction with observations of such flows, but as it turns out a fluid that rigorously satisfies all the conditions is a physical impossibility. The mathematical model breaks down at the surface of the body, and new solutions involving
boundary layers have to be considered to correctly model the drag effects.
Quantum mechanical paradoxes
A significant set of physical paradoxes are associated with the privileged position of the
observer in
quantum mechanics. Two of the most famous of these are the
EPR paradox and
Schrödinger's cat, both proposed as thought experiments relevant to the discussions of what the correct
interpretation of quantum mechanics is. These
thought experiments both try to use principles derived from the
Copenhagen interpretation of quantum mechanics to derive conclusions that are seemingly contradictory. In the case of
Schrödinger's cat this takes the form of a seeming absurdity. A cat is placed in a box sealed off from observation with a quantum mechanical switch designed to kill the cat when appropriately deployed. While in the box, the cat is described as being in a
quantum superposition of "dead" and "alive" states, though opening the box effectively collapses the cat's
wavefunction to one of the two conditions. In the case of the
EPR paradox,
quantum entanglement appears to allow for the physical impossibility of
information transmitted faster than the
speed of light, violating
special relativity.
The "resolutions" to these paradoxes are considered by many to be philosophically unsatisfying because they hinge on what is specifically meant by the
measurement of an
observation or what serves as an observer in the thought experiments. In a real physical sense, no matter what way either of those terms are defined, the results are the same. Any given observation of a cat will yield either one that is dead or alive; the superposition is a necessary condition for calculating what is to be expected, but will never itself be observed. Likewise, the
EPR paradox thought experiment yields no way of transmitting information faster than the speed of light, though there is a seemingly instantaneous conservation of the quantumly entangled observable being measured, it turns out that it is physically impossible to use this effect to transmit information. Why there is an instantaneous conservation is the subject of which is the correct
interpretation of quantum mechanics.
Speculative theories of
quantum gravity that combine
general relativity with
quantum mechanics have their own associated paradoxes that are generally accepted to be artifacts of the lack of a consistent physical model that unites the two formulations. One such paradox is the
black hole information paradox which points out that
information associated with a particle that falls into a black hole is not conserved when the theoretical
Hawking radiation causes the black hole to evaporate. In
2004,
Stephen Hawking claimed to have a working resolution to this problem, but the details have yet to be published and the speculative nature of
Hawking radiation means that it isn't clear whether this paradox is relevant to physical reality.
Causality paradoxes
A set of similar paradoxes occurs within the area of physics involving
arrow of time and
causality. One of these, the
grandfather paradox, deals with the peculiar nature of
causality in closed
time-like loops. In its most crude conception, the paradox involves a person traveling back in time and murdering an ancestor who hadn't yet had a chance to procreate. The speculative nature of time travel to the past means that there is no agreed upon resolution to the paradox, nor is it even clear that there are physically possible solutions to the
Einstein equations that would allow for the conditions required for the paradox to be met. Nevertheless, there are two common explanations for possible resolutions for this paradox that take on similar flavor for the explanations of quantum mechanical paradoxes. In the so-called
self-consistent solution,
reality is constructed in such a way as to
deterministically prevent such paradoxes from occurring. This idea makes many
free will advocates uncomfortable, though it is very satisfying to many
philosophical naturalists. Alternatively, the
many worlds idealization or the concept of
parallel universes is sometimes conjectured to allow for a continual fracturing of possible
worldlines into many different alternative realities. This would mean that any person who traveled back in time would necessarily enter a different parallel universe that would have a different history from the point of the time travel forward.
Another paradox associated with the causality and the one-way nature of time is
Loschmidt's paradox which poses the question how can microprocesses that are
time-reversible produce a
time-irreversible increase in
entropy. A partial resolution to this paradox is rigorously provided for by the
fluctuation theorem which relies on carefully keeping track of time averaged quantities to show that from a
statistical mechanics point of view, entropy is far more likely to increase than to decrease. However, if no assumptions about initial boundary conditions are made, the fluctuation theorem should apply equally well in reverse, predicting that a system currently in a low-entropy state is more likely to have been at a higher-entropy state in the past, in contradiction with what would usually be seen in a reversed film of a nonequilibrium state going to equilibrium. Thus, the overall asymmetry in thermodynamics which is at the heart of Loschmidt's paradox is still not resolved by the fluctuation theorem. Most physicists believe that the thermodynamic
arrow of time can only be explained by appealing to low entropy conditions shortly after the
big bang, although the explanation for the low entropy of the big bang itself is still debated.
Observational paradoxes
A further set of physical paradoxes are based on sets of observations that fail to be adequately explained by current physical models. These may simply be indications of the incompleteness of current theories. It is recognized that
unification has not been accomplished yet which may hint at fundamental problems with the current
scientific paradigms. Whether this is the harbinger of a
scientific revolution yet to come or whether these observations will yield to future refinements or be found to be erroneous is yet to be determined. A brief list of these yet inadequately explained observations includes observations implying the existence of
dark matter, observations implying the existence of
dark energy,
the observed matter-antimatter asymmetry, the
GZK paradox, the
quantum Smarandche paradoxes, the
Pioneer anomaly, and the
Fermi paradox.
See also
List of paradoxes
References
★
Relativity and Common Sense, Bondi, Hermann, , , Dover Publications, 1980, ISBN 0-486-24021-5
★
General Relativity from A to B, Geroch, Robert, , , University Of Chicago Press, 1981, ISBN 0-226-28864-1
★
Time Travel in Einstein's Universe, Gott, J. Richard, , , Mariner Books, 2002, ISBN 0-395-95563-7
★
Mr Tompkins in Paperback, Gamow, George, , , Cambridge University Press, 1993 (reissue edition), ISBN 0-521-44771-2
★
QED: The Strange Theory of Light and Matter, Feynman, Richard P., , , Princeton University Press, 1988, ISBN 0-691-02417-0
★
The Quantum World : Quantum Physics for Everyone, Ford, Kenneth W. and Paul Hewitt, , , Harvard University Press, 2004, ISBN 0-674-01342-5
External links
★
Usenet Physics FAQ by John Baez
★
Time travel and modern physics
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