- Physical paradox
A physical
paradox is an apparent contradiction in physical descriptions of theuniverse . While many physical paradoxes have accepted resolutions, others defy resolution and may indicate flaws in theory. Inphysics as in all of science,contradiction s andparadox es are generally assumed to be artifacts of error and incompleteness becausereality is assumed to be completely consistent, although this is itself a philosophical assumption. When, as in fields such asquantum physics andrelativity 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 ofmodern 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: thetwins paradox and theladder paradox . Both of these paradoxes involve thought experiments which defy traditionalcommon sense assumptions abouttime andspace . In particular, the effects oftime dilation andlength contraction are used in both of these paradoxes to create situations which seemingly contradict each other. It turns out that the fundamentalpostulate of special relativity that thespeed of light isinvariant in all frames of reference requires that concepts such assimultaneity andabsolute time are not applicable when comparing radically different frames of reference.Another paradox associated with relativity is
Supplee's paradox which seems to describe tworeference frame s 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 ofgeneral relativity need to be taken into account. Taking the correct assumptions, the resolution is actually a way of restating theequivalence principle .Babinet's paradox is that contrary to naive expectations, the amount of radiation removed from a beam in the
diffraction limit is equal to twice the cross-sectional area. This is because there are two separate processes which remove radiation from the beam in equal amounts:absorption anddiffraction .Similarly, there exists a set of physical paradoxes that directly rely on one or more assumptions that are incorrect. The
Gibbs paradox ofstatistical mechanics yields an apparent contradiction when calculating theentropy of mixing. If the assumption that the particles in anideal gas are indistinguishable is not appropriately taken into account, the calculated entropy is not anextensive 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 andisotropic universe as required by thecosmological 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 tonon-linear effects that influence the freezing process. The assumption that only thetemperature 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 continuity,infinitesimal s, and infinities often associated withspace andtime . For example, theelectric field associated with apoint 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 constructedDirac 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 ofquantum electrodynamics removes the need for infinitesimal point charges altogether.A similar situation occurs in
general relativity with thegravitational singularity associated with theSchwarzschild solution that describes thegeometry of ablack hole . Thecurvature ofspacetime 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 ofquantum 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 (seeBig 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 thePlanck 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 offluid mechanics . When theforce s associated withtwo-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 involvingboundary 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 theEPR paradox andSchrödinger's cat , both proposed as thought experiments relevant to the discussions of what the correctinterpretation of quantum mechanics is. Thesethought experiments both try to use principles derived from theCopenhagen interpretation of quantum mechanics to derive conclusions that are seemingly contradictory. In the case ofSchrödinger'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 aquantum superposition of "dead" and "alive" states, though opening the box effectively collapses the cat'swavefunction to one of the two conditions. In the case of theEPR paradox ,quantum entanglement appears to allow for the physical impossibility ofinformation transmitted faster than thespeed of light , violatingspecial 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 anobservation 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, theEPR 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 correctinterpretation of quantum mechanics .Speculative theories of
quantum gravity that combinegeneral relativity withquantum 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 theblack hole information paradox which points out thatinformation associated with a particle that falls into a black hole is not conserved when the theoreticalHawking radiation causes the black hole to evaporate. In2004 ,Stephen Hawking claimed to have a working resolution to this problem, but the details have yet to be published and the speculative nature ofHawking 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 andcausality . One of these, thegrandfather paradox , deals with the peculiar nature ofcausality in closedtime-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 manyfree 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 possibleworldline s 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 inentropy . A partial resolution to this paradox is rigorously provided for by thefluctuation theorem which relies on carefully keeping track of time averaged quantities to show that from astatistical 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 thermodynamicarrow of time can only be explained by appealing to low entropy conditions shortly after thebig 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 paradigm s. Whether this is the harbinger of ascientific 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 ofdark matter , observations implying the existence ofdark energy , the observed matter-antimatter asymmetry, theGZK paradox , thePioneer anomaly , and theFermi paradox .ee also
List of paradoxes References
* cite book
author = Bondi, Hermann
title = Relativity and Common Sense
publisher = Dover Publications
year = 1980
pages = 177
id = ISBN 0-486-24021-5
* cite book
author = Geroch, Robert
title = General Relativity from A to B
publisher = University Of Chicago Press
year = 1981
pages = 233
id = ISBN 0-226-28864-1
* cite book
author = Gott, J. Richard
title = Time Travel in Einstein's Universe
publisher = Mariner Books
year = 2002
pages = 291
id = ISBN 0-395-95563-7
* cite book
author = Gamow, George
title = Mr Tompkins in Paperback
publisher = Cambridge University Press
year = 1993 (reissue edition)
pages = 202
id = ISBN 0-521-44771-2
* cite book
author = Feynman, Richard P.
title = QED: The Strange Theory of Light and Matter
publisher = Princeton University Press
year = 1988
pages = 176
id = ISBN 0-691-02417-0
* cite book
author = Ford, Kenneth W. and Paul Hewitt
title = The Quantum World : Quantum Physics for Everyone
publisher = Harvard University Press
year = 2004
pages = 288
id = ISBN 0-674-01342-5External links
* [http://math.ucr.edu/home/baez/physics/ Usenet Physics FAQ by John Baez]
* [http://plato.stanford.edu/entries/time-travel-phys Time travel and modern physics]
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