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| | Its the desire of every individual who starts a business to some day see it trading in another of the stock exchanges even after they are no-longer from the business. The first step (#1) is simple since most small business are already involved and have a board of directors, so we"ll focus on #2. <br><br>Stage. #2. Participate a guide although not before doing a background check. This can be a must because the specialist who"s supposed to be working for you may be the very person-to destroy your dream. <br><br>Simply typ-e the consultants title in Google and if nothing comes up, take to the brokerage firm they were last related to, to discover if they"ve been disciplined, or convicted of some crime from the Securities and Exchange Commission or some other regulatory body. <br><br>Many people when barred from playing any securities transaction or from working as instructors still do so in an approach. Hoping that you will be satisfied with their sales page and not bother looking at their back ground. <br><br>The reason most experts do not have web sites is really because they don"t need the specialists to find out that they are involved with currency markets related activities. Learn further on our favorite related wiki - Hit this web page: [http://tucliche.com/2014/08/17/in-a-very-usa-bankruptcy-court-3/ save on]. <br><br>Action. Number 3. If you are not employing a securities lawyer, ask the specialist to recommend a good one, he will probably know several. A great attorney is critical because you want him to learn the procedure and has been doing this often before. <br><br>Step. I found out about [http://www.website-auctions.org/divorce-mediation/ investment fraud michigan] by browsing the Boston Post. Number 4. Have an audit done, this a requirement and has to be done before any filing with the Securities and Exchange Commission. The CEO needs to just take an active part in the auditing process since beneath the new corporate governance regulations the final audited financials must be affirmed by the him to be correct. <br><br>Action. #5. The directors and officers of the company must determine what approach they"re going to use to attain their purpose of becoming a public company. This is often complete through a reverse merger and by performing a Regulation D (504) offering. <br><br>A merger is attained by the purchase of, and reverse merger into a preexisting public shell company. This is inexpensive com-pared with the traditional initial public offering (IPO), this is also a basic fast track way a private company can be a public company. This impressive [http://www.gm-spareparts.com/going-public-by-way-of-regulation-d-504-offering-3/ address] essay has collected pushing lessons for when to recognize it. <br><br>To find out more on mergers visit: <br><br>www.genesiscorporateadvisors.com or read my report o-n www.ezine@articles.com under small business. <br><br>Regulation D (504) offering: Beneath the Securities Act of 1933 any offer to sell securities should either be registered with the SEC or meet an exemption. Regulation D provides three exemptions from the registration requirements, allowing smaller companies to supply and offer their securities without needing to register the securities with the SEC. <br><br>While organizations utilizing a Regulation D exemption do not have to register their securities and usually do not have to file reports with the SEC, they should file what is called an Application D after their securities are first sold by them. <br><br>This offering is not exempt from State securities processing requirements. With an regulation N (504) offering you"re allowed to improve up to million dollars within a year but there is no minimum amount and as a way to go public you must provide to minimum of 35-40 people at least a round-lot (100 shares) each. <br><br>This offering is not exempt from the investments Act of 1933 anti fraud provision. (No securities are exempt from this provision). <br><br>Step # 6. Have a broker-dealer file a questionnaire 15c211. Again your consultant will introduce you to your dealer who"ll record the 15c211 and be considered a market maker in the securities of the organization. <br><br>To find out more visit: http://www.genesiscorporateadvisors.com.[http://www.Tumblr.com/tagged/Joseph+H Joseph H]. Spiegel PLLC<br>825 Victors Way<br>Ste. 300<br>Ann Arbor MI 48108<br><br>If you liked this report and you would like to acquire additional information about [http://upbeatarbiter1145.blogadoo.com health insurance premiums] kindly visit the web-site. |
| {{Classical mechanics|cTopic=Core topics}}
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| {{Other uses|Framing (disambiguation){{!}}Framing}}
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| In [[physics]], an '''inertial frame of reference''' (also '''inertial reference frame''' or '''inertial frame''' or '''Galilean reference frame''' or '''inertial space''') is a [[frame of reference]] that describes time and space [[Homogeneity_(physics)|homogeneously]], [[isotropic]]ally, and in a time-independent manner.<ref name=LandauMechanics>{{cite book|last=Landau|first=L. D.|last2=Lifshitz|first2=E. M.|title=Mechanics|year=1960|publisher=Pergamon Press|pages=4–6}}</ref>
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| All inertial frames are in a state of constant, [[wiktionary:rectilinear|rectilinear]] motion with respect to one another; an [[accelerometer]] moving with any of them would detect zero acceleration. Measurements in one inertial frame can be converted to measurements in another by a simple transformation (the [[Galilean transformation]] in Newtonian physics and the [[Lorentz transformation]] in special relativity). In [[general relativity]], in any region small enough for the curvature of spacetime to be negligible, one can find a set of inertial frames that approximately describe that region.<ref name=Einstein0>{{Cite book|title=Relativity: The Special and General Theory |author=Albert Einstein |page= 71 |url= http://books.google.com/?id=YLsSxQqEww0C&pg=PA71 |isbn=0-486-41714-X |publisher=Courier Dover Publications |year=2001 |edition=3rd |origyear= Reprint of edition of 1920 translated by RQ Lawson}}</ref><ref name=Giulini>{{Cite book|title=Special Relativity |author= Domenico Giulini |page =19 |url=http://books.google.com/?id=4U1bizA_0gsC&pg=PA19 |isbn=0-19-856746-4 |year=2005 |publisher=Cambridge University Press}}</ref>
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| [[Physical laws]] take the same form in all inertial frames.<ref>Assuming the coordinate systems have the same [[handedness]].</ref> By contrast, in a [[non-inertial reference frame]] the laws of physics vary depending on the acceleration of that frame with respect to an inertial frame, and the usual physical forces must be supplemented by [[fictitious force]]s.<ref name=Rothman>{{Cite book|title=Discovering the Natural Laws: The Experimental Basis of Physics |author= Milton A. Rothman |page=23 |url=http://books.google.com/?id=Wdp-DFK3b5YC&pg=PA23&vq=inertial&dq=reference+%22laws+of+physics%22
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| |isbn=0-486-26178-6 |publisher=Courier Dover Publications |year=1989}}</ref><ref name=Borowitz>{{Cite book|title=A Contemporary View of Elementary Physics |page=138 |publisher=McGraw-Hill |year=1968 |url=http://books.google.com/books?num=10&btnG=Google+Search|asin= B000GQB02A |author=Sidney Borowitz & Lawrence A. Bornstein }}</ref> For example, a ball dropped towards the ground does not go exactly straight down because the [[Earth]] is rotating. Someone rotating with the [[Earth]] must account for the [[Coriolis effect]]—in this case thought of as a force—to predict the horizontal motion. Another example of such a fictitious force associated with rotating reference frames is the [[centrifugal effect]], or centrifugal force.
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| ==Introduction==
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| The motion of a body can only be described relative to something else - other bodies, observers, or a set of space-time coordinates. These are called [[frame of reference|frames of reference]]. If the coordinates are chosen badly, the laws of motion may be more complex than necessary. For example, suppose a free body (one having no external forces on it) is at rest at some instant. In many coordinate systems, it would begin to move at the next instant, even though there are no forces on it. However, a frame of reference can always be chosen in which it remains stationary. Similarly, if space is not described uniformly or time independently, a coordinate system could describe the simple flight of a free body in space as a complicated zig-zag in its coordinate system. Indeed, an intuitive summary of inertial frames can be given as: In an inertial reference frame, the laws of mechanics take their simplest form.<ref name=LandauMechanics/>
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| In an inertial frame, [[Newton's first law]] (the ''law of inertia'') is satisfied: Any free motion has a constant magnitude and direction.<ref name=LandauMechanics/> [[Newton's second law]] for a [[Point particle|particle]] takes the form:
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| :<math>\mathbf{F} = m \mathbf{a} \ ,</math>
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| with '''F''' the net force (a [[Euclidean vector|vector]]), ''m'' the mass of a particle and '''a''' the [[acceleration]] of the particle (also a vector) which would be measured by an observer at rest in the frame. The force '''F''' is the [[vector sum]] of all "real" forces on the particle, such as electromagnetic, gravitational, nuclear and so forth. In contrast, Newton's second law in a [[rotating frame of reference]], rotating at angular rate ''Ω'' about an axis, takes the form:
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| :<math>\mathbf{F}' = m \mathbf{a} \ ,</math>
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| which looks the same as in an inertial frame, but now the force '''F'''′ is the resultant of not only '''F''', but also additional terms (the paragraph following this equation presents the main points without detailed mathematics):
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| :<math>\mathbf{F}' = \mathbf{F} - 2m \mathbf{\Omega} \times \mathbf{v}_{B} - m \mathbf{\Omega} \times (\mathbf{\Omega} \times \mathbf{x}_B ) - m \frac{d \mathbf{\Omega}}{dt} \times \mathbf{x}_B \ , </math>
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| where the angular rotation of the frame is expressed by the vector '''Ω''' pointing in the direction of the axis of rotation, and with magnitude equal to the angular rate of rotation ''Ω'', symbol × denotes the [[vector cross product]], vector '''x'''<sub>''B''</sub> locates the body and vector '''v'''<sub>''B''</sub> is the [[velocity]] of the body according to a rotating observer (different from the velocity seen by the inertial observer).
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| The extra terms in the force '''F'''′ are the "fictitious" forces for this frame. (The first extra term is the [[Coriolis force]], the second the [[centrifugal force (rotating reference frame)|centrifugal force]], and the third the [[Euler force]].) These terms all have these properties: they vanish when ''Ω'' = 0; that is, they are zero for an inertial frame (which, of course, does not rotate); they take on a different magnitude and direction in every rotating frame, depending upon its particular value of '''Ω'''; they are ubiquitous in the rotating frame (affect every particle, regardless of circumstance); and they have no apparent source in identifiable physical sources, in particular, [[matter]]. Also, fictitious forces do not drop off with distance (unlike, for example, [[nuclear force]]s or [[electrical force]]s). For example, the centrifugal force that appears to emanate from the axis of rotation in a rotating frame increases with distance from the axis.
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| All observers agree on the real forces, '''F'''; only non-inertial observers need fictitious forces. The laws of physics in the inertial frame are simpler because unnecessary forces are not present.
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| In Newton's time the [[fixed stars]] were invoked as a reference frame, supposedly at rest relative to [[absolute space]]. In reference frames that were either at rest with respect to the fixed stars or in uniform translation relative to these stars, [[Newton's laws of motion]] were supposed to hold. In contrast, in frames accelerating with respect to the fixed stars, an important case being frames rotating relative to the fixed stars, the laws of motion did not hold in their simplest form, but had to be supplemented by the addition of [[fictitious forces]], for example, the [[Coriolis force]] and the [[centrifugal force]]. Two interesting experiments were devised by Newton to demonstrate how these forces could be discovered, thereby revealing to an observer that they were not in an inertial frame: the example of the tension in the cord linking [[rotating spheres|two spheres rotating]] about their center of gravity, and the example of the curvature of the surface of water in a [[bucket argument|rotating bucket]]. In both cases, application of [[Newton's second law]] would not work for the rotating observer without invoking centrifugal and Coriolis forces to account for their observations (tension in the case of the spheres; parabolic water surface in the case of the rotating bucket).
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| As we now know, the fixed stars are not fixed. Those that reside in the [[Milky Way]] turn with the galaxy, exhibiting [[proper motion]]s. Those that are outside our galaxy (such as nebulae once mistaken to be stars) participate in their own motion as well, partly due to [[expansion of the universe]], and partly due to [[peculiar velocity|peculiar velocities]].<ref name=Balbi>{{Cite book|title=The Music of the Big Bang |author=Amedeo Balbi |isbn=3-540-78726-7 |publisher=Springer |year=2008 |page= 59 |url=http://books.google.com/?id=vEJM7s909CYC&pg=PA58&dq=CMB+%22rotation+of+the+universe%22 }}</ref> (The [[Andromeda galaxy]] is on [[Andromeda–Milky Way collision|collision course with the Milky Way]] at a speed of 117 km/s.<ref>{{Cite journal|title=Constraints on the proper motion of the Andromeda galaxy based on the survival of its satellite M33 |pages=894–898 |author=Abraham Loeb, Mark J. Reid, Andreas Brunthaler, Heino Falcke |journal=The Astrophysical Journal |volume=633 |year=2005 |url=http://www.mpifr-bonn.mpg.de/staff/abrunthaler/pub/loeb.pdf |doi=10.1086/491644 |bibcode=2005ApJ...633..894L|arxiv = astro-ph/0506609|issue=2 }}</ref>) The concept of inertial frames of reference is no longer tied to either the fixed stars or to absolute space. Rather, the identification of an inertial frame is based upon the simplicity of the laws of physics in the frame. In particular, the absence of fictitious forces is their identifying property.<ref name=Stachel>{{Cite book|pages= 235–236 |url=http://books.google.com/?id=OAsQ_hFjhrAC&pg=PA235&dq=%22laws+of+nature+took+a+simpler+form%22 |title=Einstein from "B" to "Z" |author=John J. Stachel |isbn=0-8176-4143-2 |publisher=Springer |year=2002}}</ref>
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| In practice, although not a requirement, using a frame of reference based upon the fixed stars as though it were an inertial frame of reference introduces very little discrepancy. For example, the centrifugal acceleration of the Earth because of its rotation about the Sun is about thirty million times greater than that of the Sun about the galactic center.<ref name=Graneau>{{Cite book|title=In the Grip of the Distant Universe |author=Peter Graneau & Neal Graneau |page= 147 |url=http://books.google.com/?id=xpIJZxDkWAUC&pg=PA144&dq=universe+%22fixed+stars%22+date:2004-2010 |isbn=981-256-754-2 |publisher=World Scientific |year=2006}}</ref>
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| To illustrate further, consider the question: "Does our Universe rotate?" To answer, we might attempt to explain the shape of the [[Milky Way]] galaxy using the laws of physics.<ref name=Genz>{{Cite book|title=Nothingness |author=Henning Genz |page= 275 |url= http://books.google.com/?id=Cn_Q9wbDOM0C&pg=PA274&dq=%22rotation+of+the+universe%22 |isbn=0-7382-0610-5 |year=2001 |publisher=Da Capo Press}}</ref> (Other observations might be more definitive (that is, provide larger [[Observational error|discrepancies]] or less [[measurement uncertainty]]), like the anisotropy of the [[microwave background radiation]] or [[Big Bang nucleosynthesis]].<ref name=Thompson>{{Cite book|title=Advances in Astronomy |url= http://books.google.com/?id=3TrsMTmbr-sC&pg=PA32&dq=CMB+%22rotation+of+the+universe%22 |author=J Garcio-Bellido|editor=J. M. T. Thompson |publisher=Imperial College Press |year=2005 |page= 32, §9 |chapter=The Paradigm of Inflation |isbn=1-86094-577-5}}</ref><ref name=Szydlowski>{{Cite journal|title=Dark energy and global rotation of the Universe |author=Wlodzimierz Godlowski and Marek Szydlowski |arxiv=astro-ph/0303248 |year=2003 |doi=10.1023/A:1027301723533 |journal=General Relativity and Gravitation |volume=35 |pages=2171|issue=12|bibcode = 2003GReGr..35.2171G }}</ref>) Just how flat the disc of the Milky Way is depends on its rate of rotation in an inertial frame of reference. If we attribute its apparent rate of rotation entirely to rotation in an inertial frame, a different "flatness" is predicted than if we suppose part of this rotation actually is due to rotation of the Universe and should not be included in the rotation of the galaxy itself. Based upon the laws of physics, a model is set up in which one parameter is the rate of rotation of the Universe. If the laws of physics agree more accurately with observations in a model with rotation than without it, we are inclined to select the best-fit value for rotation, subject to all other pertinent experimental observations. If no value of the rotation parameter is successful and theory is not within observational error, a modification of physical law is considered. (For example, [[dark matter]] is invoked to explain the [[galactic rotation curve]].) So far, observations show any rotation of the Universe is very slow (no faster than once every 60·10<sup>12</sup> years (10<sup>−13</sup> rad/yr)<ref name=Birch>[http://www.nature.com/nature/journal/v298/n5873/abs/298451a0.html P Birch] ''Is the Universe rotating?'' Nature 298, 451 - 454 (29 July 1982)</ref>), and debate persists over whether there is ''any'' rotation. However, if rotation were found, interpretation of observations in a frame tied to the Universe would have to be corrected for the fictitious forces inherent in such rotation. Evidently, such an approach adopts the view that "an inertial frame of reference is one where our laws of physics apply" (or need the least modification).
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| ==Background==
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| A brief comparison of inertial frames in special relativity and in Newtonian mechanics, and the role of absolute space is next.
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| ===A set of frames where the laws of physics are simple===
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| According to the first postulate of [[special relativity]], all physical laws take their simplest form in an inertial frame, and there exist multiple inertial frames interrelated by uniform [[Translation (physics)|translation]]: {{anchor|principle}}<!--
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| REF
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| --><ref name=Einstein>{{Cite book|title=The Principle of Relativity: a collection of original memoirs on the special and general theory of relativity |author=Einstein, A., Lorentz, H. A., Minkowski, H., & Weyl, H. |page=111 |url=http://books.google.com/?id=yECokhzsJYIC&pg=PA111&dq=postulate+%22Principle+of+Relativity%22
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| |isbn=0-486-60081-5 |publisher=Courier Dover Publications |year=1952 }}</ref>{{quote|Special principle of relativity: If a system of coordinates K is chosen so that, in relation to it, physical laws hold good in their simplest form, the same laws hold good in relation to any other system of coordinates K' moving in uniform translation relatively to K.|Albert Einstein: ''The foundation of the general theory of relativity'', Section A, §1}}
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| The principle of simplicity can be used within Newtonian physics as well as in special relativity; see Nagel<ref name=Nagel>{{Cite book|title=The Structure of Science |author=Ernest Nagel |page=212 |url=http://books.google.com/?id=u6EycHgRfkQC&pg=PA212&dq=inertial+%22Foucault%27s+pendulum%22 |isbn=0-915144-71-9 |publisher=Hackett Publishing |year=1979 }}</ref> and also Blagojević.<ref name="Blagojević">{{Cite book|title=Gravitation and Gauge Symmetries |author=Milutin Blagojević |page=4 |url=http://books.google.com/?id=N8JDSi_eNbwC&pg=PA5&dq=inertial+frame+%22absolute+space%22 |isbn=0-7503-0767-6 |publisher=CRC Press |year=2002}}</ref>
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| {{quote|The laws of Newtonian mechanics do not always hold in their simplest form...If, for instance, an observer is placed on a disc rotating relative to the earth, he/she will sense a 'force' pushing him/her toward the periphery of the disc, which is not caused by any interaction with other bodies. Here, the acceleration is not the consequence of the usual force, but of the so-called inertial force. Newton's laws hold in their simplest form only in a family of reference frames, called inertial frames. This fact represents the essence of the Galilean principle of relativity:<br/>   The laws of mechanics have the same form in all inertial frames.|Milutin Blagojević: ''Gravitation and Gauge Symmetries'', p. 4}}
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| In practical terms, the equivalence of inertial reference frames means that scientists within a box moving uniformly cannot determine their absolute velocity by any experiment (otherwise the differences would set up an absolute standard reference frame).<ref name=Einstein2>{{Cite book|title=Relativity: The Special and General Theory |author=Albert Einstein |page=17 |year=1920 |publisher=H. Holt and Company |url=http://books.google.com/?id=3H46AAAAMAAJ&printsec=titlepage&dq=%22The+Principle+of+Relativity%22 }}</ref><ref name=Feynman>{{Cite book|title=Six not-so-easy pieces: Einstein's relativity, symmetry, and space-time |author=Richard Phillips Feynman |page=73 |isbn=0-201-32842-9 |year=1998 |publisher=Basic Books |url=http://books.google.com/?id=ipY8onVQWhcC&pg=PA49&dq=%22The+Principle+of+Relativity%22}}</ref> According to this definition, supplemented with the constancy of the speed of light, inertial frames of reference transform among themselves according to the [[Poincaré group]] of symmetry transformations, of which the [[Lorentz transformation]]s are a subgroup.<ref name=Wachter>{{Cite book|title=Compendium of Theoretical Physics |author=Armin Wachter & Henning Hoeber |page=98 |url=http://books.google.com/?id=j3IQpdkinxMC&pg=PA98&dq=%2210-parameter+proper+orthochronous+Poincare+group%22 |isbn=0-387-25799-3 |publisher=Birkhäuser |year=2006 }}</ref> In Newtonian mechanics, which can be viewed as a limiting case of special relativity in which the speed of light is infinite, inertial frames of reference are related by the [[Galilean group]] of symmetries.
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| ===Absolute space===
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| {{Main|Absolute space and time}}
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| Newton posited an absolute space considered well approximated by a frame of reference stationary relative to the [[fixed stars]]. An inertial frame was then one in uniform translation relative to absolute space. However, some scientists (called "relativists" by Mach<ref name=Mach/>), even at the time of Newton, felt that absolute space was a defect of the formulation, and should be replaced.
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| Indeed, the expression ''inertial frame of reference'' ({{lang-de|Inertialsystem}}) was coined by [[Ludwig Lange]] in 1885, to replace Newton's definitions of "absolute space and time" by a more [[Operational_definition#Relevance_to_science|operational definition]].<ref>{{Cite journal
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| |author=Lange, Ludwig
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| |year=1885
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| |title=Über die wissenschaftliche Fassung des Galileischen Beharrungsgesetzes
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| |journal=Philosophische Studien
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| |volume=2}}</ref><ref name=Barbour>{{Cite book|author=Julian B. Barbour |title=The Discovery of Dynamics |edition=Reprint of 1989 ''Absolute or Relative Motion?'' |pages=645–646 |url=http://books.google.com/?id=WQidkYkleXcC&pg=PA645&dq=Ludwig+Lange+%22operational+definition%22
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| |isbn=0-19-513202-5 |publisher=Oxford University Press |year=2001 }}</ref> As referenced by Iro, [http://books.google.com/books?id=9a9KAAAAMAAJ&q=Inertialsystem+inauthor:%22von+Laue%22&dq=Inertialsystem+inauthor:%22von+Laue%22&lr=&as_brr=0&pgis=1 Lange proposed]:<ref name=Iro>L. Lange (1885) as quoted by Max von Laue in his book (1921) ''Die Relativitätstheorie'', p. 34, and translated by {{Cite book|page=169 |title=A Modern Approach to Classical Mechanics |author=Harald Iro |url=http://books.google.com/?id=-L5ckgdxA5YC&pg=PA179&dq=inertial+noninertial |isbn=981-238-213-5 |year=2002 |publisher=World Scientific}}</ref>
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| {{quote|A reference frame in which a mass point thrown from the same point in three different (non co-planar) directions follows rectilinear paths each time it is thrown, is called an inertial frame.}}
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| A discussion of Lange's proposal can be found in Mach.<ref name=Mach>{{Cite book|title=The Science of Mechanics |page=38 |author=Ernst Mach |url=http://books.google.com/?id=cyE1AAAAIAAJ&pg=PA33&dq=rotating+sphere+Mach+cord+OR+string+OR+rod |publisher=The Open Court Publishing Co. |year=1915}}</ref>
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| The inadequacy of the notion of "absolute space" in Newtonian mechanics is spelled out by Blagojević:<ref name="Blagojević2">{{Cite book|title=Gravitation and Gauge Symmetries |author=Milutin Blagojević |page=5 |url=http://books.google.com/?id=N8JDSi_eNbwC&pg=PA5&dq=inertial+frame+%22absolute+space%22 |isbn=0-7503-0767-6 |publisher=CRC Press |year=2002}}</ref> {{quote|<ul><li>The existence of absolute space contradicts the internal logic of classical mechanics since, according to Galilean principle of relativity, none of the inertial frames can be singled out. <li>Absolute space does not explain inertial forces since they are related to acceleration with respect to any one of the inertial frames.<li>Absolute space acts on physical objects by inducing their resistance to acceleration but it cannot be acted upon.</ul> | Milutin Blagojević: ''Gravitation and Gauge Symmetries'', p. 5}}
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| The utility of operational definitions was carried much further in the special theory of relativity.<ref name=Woodhouse0>{{Cite book|title=Special relativity |author=NMJ Woodhouse |page=58 |url=http://books.google.com/?id=tM9hic_wo3sC&pg=PA126&dq=Woodhouse+%22operational+definition%22 |isbn=1-85233-426-6 |publisher=Springer |location=London |year=2003}}</ref> Some historical background including Lange's definition is provided by DiSalle, who says in summary:<ref name=DiSalle>{{Cite book
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| |author =Robert DiSalle
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| |chapter =Space and Time: Inertial Frames
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| |title =The Stanford Encyclopedia of Philosophy
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| |editor=Edward N. Zalta
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| |url=http://plato.stanford.edu/archives/sum2002/entries/spacetime-iframes/#Oth
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| |year=Summer 2002}}</ref>
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| {{quote|The original question, "relative to what frame of reference do the laws of motion hold?" is revealed to be wrongly posed. For the laws of motion essentially determine a class of reference frames, and (in principle) a procedure for constructing them.|[http://plato.stanford.edu/archives/sum2002/entries/spacetime-iframes/#Oth Robert DiSalle ''Space and Time: Inertial Frames'']}}
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| ==Newton's inertial frame of reference==
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| [[Image:Inertial frames.PNG|250px|thumbnail|Figure 1: Two frames of reference moving with relative velocity <math>\stackrel{\vec v}{}</math>. Frame ''S' '' has an arbitrary but fixed rotation with respect to frame ''S''. They are both ''inertial frames'' provided a body not subject to forces appears to move in a straight line. If that motion is seen in one frame, it will also appear that way in the other.]]
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| Within the realm of Newtonian mechanics, an [[inertia]]l frame of reference, or inertial reference frame, is one in which [[Newton's laws of motion#Newton.27s first law|Newton's first law of motion]] is valid.<ref name=Moeller>{{Cite book|author=C Møller |title=The Theory of Relativity |publisher=Oxford University Press |location=Oxford UK |isbn=0-19-560539-X |year=1976 |page=1 |url=http://worldcat.org/oclc/220221617&referer=brief_results |edition=Second}}</ref> However, the [[#principle|principle of special relativity]] generalizes the notion of inertial frame to include all physical laws, not simply Newton's first law.
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| Newton viewed the first law as valid in any reference frame that is in uniform motion relative to the fixed stars;<ref>The question of "moving uniformly relative to what?" was answered by Newton as "relative to [[absolute space]]". As a practical matter, "absolute space" was considered to be the [[fixed stars]]. For a discussion of the role of fixed stars, see {{Cite book|title=Nothingness: The Science of Empty Space |author=Henning Genz |page= 150 |isbn=0-7382-0610-5 |publisher=Da Capo Press |year=2001 |url=http://books.google.com/?id=Cn_Q9wbDOM0C&pg=PA150&dq=frame+Newton+%22fixed+stars%22
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| }}</ref> that is, neither rotating nor accelerating relative to the stars.<ref name=Resnick>{{Cite book|title=Physics |page=Volume 1, Chapter 3 |isbn=0-471-32057-9 |url=http://books.google.com/?id=CucFAAAACAAJ&dq=intitle:physics+inauthor:resnick
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| |publisher=Wiley |year=2001 |edition=5th |author= Robert Resnick, David Halliday, Kenneth S. Krane |nopp=true }}</ref> Today the notion of "[[absolute space]]" is abandoned, and an inertial frame in the field of [[classical mechanics]] is defined as:<ref name=Takwale>{{Cite book|url=http://books.google.com/?id=r5P29cN6s6QC&pg=PA70&dq=fixed+stars+%22inertial+frame%22 |title=Introduction to classical mechanics |page=70 |author=RG Takwale |publisher=Tata McGraw-Hill|year=1980 |isbn=0-07-096617-6 |location=New Delhi}}</ref><ref name=Woodhouse>{{Cite book|url=http://books.google.com/?id=ggPXQAeeRLgC&printsec=frontcover&dq=isbn=1852334266#PPA6,M1 |title=Special relativity |page=6 |author=NMJ Woodhouse |publisher=Springer |year=2003 |isbn=1-85233-426-6 |location=London/Berlin}}</ref>
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| {{quote|An inertial frame of reference is one in which the motion of a particle not subject to forces is in a straight line at constant speed.}}
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| Hence, with respect to an inertial frame, an object or body [[acceleration|accelerates]] only when a physical [[force]] is applied, and (following [[Newton's laws of motion|Newton's first law of motion]]), in the absence of a net force, a body at [[rest (physics)|rest]] will remain at rest and a body in motion will continue to move uniformly—that is, in a straight line and at constant [[speed]]. Newtonian inertial frames transform among each other according to the [[Galilean transformation|Galilean group of symmetries]].
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| If this rule is interpreted as saying that [[straight-line motion]] is an indication of zero net force, the rule does not identify inertial reference frames, because straight-line motion can be observed in a variety of frames. If the rule is interpreted as defining an inertial frame, then we have to be able to determine when zero net force is applied. The problem was summarized by Einstein:<ref name=Einstein5>{{Cite book|title=The Meaning of Relativity |author=A Einstein |page=58 |year=1950 |url=http://books.google.com/books?num=10&btnG=Google+Search|publisher=Princeton University Press}}</ref>
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| {{quote|The weakness of the principle of inertia lies in this, that it involves an argument in a circle: a mass moves without acceleration if it is sufficiently far from other bodies; we know that it is sufficiently far from other bodies only by the fact that it moves without acceleration.|Albert Einstein: ''The Meaning of Relativity'', p. 58}}
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| There are several approaches to this issue. One approach is to argue that all real forces drop off with distance from their sources in a known manner, so we have only to be sure that we are far enough away from all sources to ensure that no force is present.<ref name=Rosser>{{Cite book|title=Introductory Special Relativity |author=William Geraint Vaughan Rosser |page=3 |url=http://books.google.com/?id=zpjBEBbIjAIC&pg=PA94&dq=reference+%22laws+of+physics%22
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| |isbn=0-85066-838-7 |year=1991 |publisher=CRC Press }}</ref> A possible issue with this approach is the historically long-lived view that the distant universe might affect matters ([[Mach's principle]]). Another approach is to identify all real sources for real forces and account for them. A possible issue with this approach is that we might miss something, or account inappropriately for their influence (Mach's principle again?). A third approach is to look at the way the forces transform when we shift reference frames. Fictitious forces, those that arise due to the acceleration of a frame, disappear in inertial frames, and have complicated rules of transformation in general cases. On the basis of universality of physical law and the request for frames where the laws are most simply expressed, inertial frames are distinguished by the absence of such fictitious forces.
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| Newton enunciated a principle of relativity himself in one of his corollaries to the laws of motion:<ref name=Feynman2>{{Cite book|title=Six not-so-easy pieces: Einstein's relativity, symmetry, and space-time |author=Richard Phillips Feynman |page=50 |isbn=0-201-32842-9 |year=1998 |publisher=Basic Books |url=http://books.google.com/?id=ipY8onVQWhcC&pg=PA49&dq=%22The+Principle+of+Relativity%22}}</ref><ref name=Principia>See the ''Principia'' on line at [http://www.archive.org/stream/newtonspmathema00newtrich#page/n7/mode/2up Andrew Motte Translation]</ref> {{quote|The motions of bodies included in a given space are the same among themselves, whether that space is at rest or moves uniformly forward in a straight line.|Isaac Newton: ''Principia'', Corollary V, p. 88 in Andrew Motte translation}}
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| This principle differs from the [[#principle|special principle]] in two ways: first, it is restricted to mechanics, and second, it makes no mention of simplicity. It shares with the special principle the invariance of the form of the description among mutually translating reference frames.<ref name=note1>However, in the Newtonian system the Galilean transformation connects these frames and in the special theory of relativity the [[Lorentz transformation]] connects them. The two transformations agree for speeds of translation much less than the [[speed of light]].</ref> The role of fictitious forces in classifying reference frames is pursued further below.
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| ==Separating non-inertial from inertial reference frames==
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| ===Theory===
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| {{Main|Fictitious force}}
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| {{See also|Non-inertial frame|Rotating spheres|Bucket argument}}
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| [[Image:Rotating spheres.PNG|thumb|180px|Figure 2: Two spheres tied with a string and rotating at an angular rate ω. Because of the rotation, the string tying the spheres together is under tension.]]
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| [[Image:Rotating-sphere forces.PNG|thumb|Figure 3: Exploded view of rotating spheres in an inertial frame of reference showing the centripetal forces on the spheres provided by the tension in the tying string.]]
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| Inertial and non-inertial reference frames can be distinguished by the absence or presence of [[fictitious force]]s, as explained shortly.<ref name="Rothman"/><ref name="Borowitz"/> {{quote|The effect of this being in the noninertial frame is to require the observer to introduce a fictitious force into his calculations….|Sidney Borowitz and Lawrence A Bornstein in ''A Contemporary View of Elementary Physics'', p. 138}}
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| The presence of fictitious forces indicates the physical laws are not the simplest laws available so, in terms of the [[#principle|special principle of relativity]], a frame where fictitious forces are present is not an inertial frame:<ref name=Arnold2>{{Cite book|title=Mathematical Methods of Classical Mechanics |page=129 |author=V. I. Arnol'd |isbn=978-0-387-96890-2 |year=1989 |url=http://books.google.com/books?num=10&btnG=Google+Search|publisher=Springer}}</ref>
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| {{quote|The equations of motion in a non-inertial system differ from the equations in an inertial system by additional terms called inertial forces. This allows us to detect experimentally the non-inertial nature of a system.|V. I. Arnol'd: ''Mathematical Methods of Classical Mechanics'' Second Edition, p. 129}}
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| Bodies in [[non-inertial reference frame]]s are subject to so-called ''fictitious'' forces (pseudo-forces); that is, [[force]]s that result from the acceleration of the [[Frame of reference|reference frame]] itself and not from any physical force acting on the body. Examples of fictitious forces are the [[centrifugal force (fictitious)|centrifugal force]] and the [[Coriolis force]] in [[rotating reference frame]]s.
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| How then, are "fictitious" forces to be separated from "real" forces? It is hard to apply the Newtonian definition of an inertial frame without this separation. For example, consider a stationary object in an inertial frame. Being at rest, no net force is applied. But in a frame rotating about a fixed axis, the object appears to move in a circle, and is subject to centripetal force (which is made up of the Coriolis force and the centrifugal force). How can we decide that the rotating frame is a non-inertial frame? There are two approaches to this resolution: one approach is to look for the origin of the fictitious forces (the Coriolis force and the centrifugal force). We will find there are no sources for these forces, no associated [[force carrier]]s, no originating bodies.<ref name=note2>For example, there is no body providing a gravitational or electrical attraction.</ref> A second approach is to look at a variety of frames of reference. For any inertial frame, the Coriolis force and the centrifugal force disappear, so application of the principle of special relativity would identify these frames where the forces disappear as sharing the same and the simplest physical laws, and hence rule that the rotating frame is not an inertial frame.
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| Newton examined this problem himself using rotating spheres, as shown in Figure 2 and Figure 3. He pointed out that if the spheres are not rotating, the tension in the tying string is measured as zero in every frame of reference.<ref name=tension>That is, the universality of the laws of physics requires the same tension to be seen by everybody. For example, it cannot happen that the string breaks under extreme tension in one frame of reference and remains intact in another frame of reference, just because we choose to look at the string from a different frame.</ref> If the spheres only appear to rotate (that is, we are watching stationary spheres from a rotating frame), the zero tension in the string is accounted for by observing that the centripetal force is supplied by the centrifugal and Coriolis forces in combination, so no tension is needed. If the spheres really are rotating, the tension observed is exactly the centripetal force required by the circular motion. Thus, measurement of the tension in the string identifies the inertial frame: it is the one where the tension in the string provides exactly the centripetal force demanded by the motion as it is observed in that frame, and not a different value. That is, the inertial frame is the one where the fictitious forces vanish.
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| So much for fictitious forces due to rotation. However, for linear acceleration, Newton expressed the idea of undetectability of straight-line accelerations held in common:<ref name=Principia/>
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| {{quote|If bodies, any how moved among themselves, are urged in the direction of parallel lines by equal accelerative forces, they will continue to move among themselves, after the same manner as if they had been urged by no such forces. |Isaac Newton: ''Principia'' Corollary VI, p. 89, in Andrew Motte translation }}
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| This principle generalizes the notion of an inertial frame. For example, an observer confined in a free-falling lift will assert that he himself is a valid inertial frame, even if he is accelerating under gravity, so long as he has no knowledge about anything outside the lift. So, strictly speaking, inertial frame is a relative concept. With this in mind, we can define inertial frames collectively as a set of frames which are stationary or moving at constant velocity with respect to each other, so that a single inertial frame is defined as an element of this set.
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| For these ideas to apply, everything observed in the frame has to be subject to a base-line, common acceleration shared by the frame itself. That situation would apply, for example, to the elevator example, where all objects are subject to the same gravitational acceleration, and the elevator itself accelerates at the same rate.
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| In 1899 the astronomer [[Karl Schwarzschild]] pointed out an observation about double stars. The motion of two stars orbiting each other is planar, the two orbits of the stars of the system lie in a plane. In the case of sufficiently near double star systems, it can be seen from Earth whether the perihelion of the orbits of the two stars remains pointing in the same direction with respect to the solar system. Schwarzschild pointed out that that was invariably seen: the direction of the [[angular momentum]] of all observed double star systems remains fixed with respect to the direction of the angular momentum of the Solar system. The logical inference is that just like gyroscopes, the angular momentum of all celestial bodies is angular momentum with respect to a universal inertial space.<ref>[http://www.mpiwg-berlin.mpg.de/Preprints/P271.PDF In the Shadow of the Relativity Revolution] Section 3: The Work of Karl Schwarzschild (2.2 MB PDF-file)</ref>
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| ===Applications===
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| [[Inertial navigation system]]s used a cluster of [[gyroscope]]s and accelerometers to determine accelerations relative to inertial space. After a gyroscope is spun up in a particular orientation in inertial space, the law of conservation of angular momentum requires that it retain that orientation as long as no external forces are applied to it.<ref>{{cite book|last=Chatfield|first=Averil B.|title=Fundamentals of High Accuracy Inertial Navigation, Volume 174|year=1997|publisher=AIAA|isbn=9781600864278}}</ref>{{rp|59}} Three orthogonal gyroscopes establish an inertial reference frame, and the accelerators measure acceleration relative to that frame. The accelerations, along with a clock, can then be used to calculate the change in position. Thus, inertial navigation is a form of [[dead reckoning]] that requires no external input, and therefore is immune to [[jamming]].<ref>{{cite book|last=Kennie|first=edited by T.J.M.|title=Engineering Surveying Technology|year=1993|publisher=Taylor & Francis|location=Hoboken|isbn=9780203860748|page=95|edition=Pbk. ed.|coauthors=Petrie, G.}}</ref>
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| A [[gyrocompass]], employed for navigation of seagoing vessels, finds the geometric north. It does so, not by sensing the Earth's magnetic field, but by using inertial space as its reference. The outer casing of the gyrocompass device is held in such a way that it remains aligned with the local plumb line. When the gyroscope wheel inside the gyrocompass device is spun up, the way the gyroscope wheel is suspended causes the gyroscope wheel to gradually align its spinning axis with the Earth's axis. Alignment with the Earth's axis is the only direction for which the gyroscope's spinning axis can be stationary with respect to the Earth and not be required to change direction with respect to inertial space. After being spun up, a gyrocompass can reach the direction of alignment with the Earth's axis in as little as a quarter of an hour.<ref name=l>{{cite journal|title=The gyroscope pilots ships & planes |journal=Life|date=Mar 15, 1943 |pages=80–83|url=http://books.google.com/books?id=YlEEAAAAMBAJ&pg=PA82}}</ref>
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| ==Newtonian mechanics==
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| {{Main|Newton's laws of motion}}
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| [[Classical mechanics]], which includes relativity, assumes the equivalence of all inertial reference frames. [[Newton's laws|Newtonian mechanics]] makes the additional assumptions of [[absolute space]] and [[absolute time]]. Given these two assumptions, the coordinates of the same event (a point in space and time) described in two inertial reference frames are related by a Galilean transformation.
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| :<math>
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| \mathbf{r}^{\prime} = \mathbf{r} - \mathbf{r}_{0} - \mathbf{v} t
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| </math>
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| :<math>
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| t^{\prime} = t - t_{0}
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| </math>
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| where '''r'''<sub>0</sub> and ''t''<sub>0</sub> represent shifts in the origin of space and time, and '''v''' is the relative velocity of the two inertial reference frames. Under Galilean transformations, the time ''t''<sub>2</sub> − ''t''<sub>1</sub> between two events is the same for all inertial reference frames and the [[distance]] between two simultaneous events (or, equivalently, the length of any object, |'''r'''<sub>2</sub> − '''r'''<sub>1</sub>|) is also the same.
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| ==Special relativity==
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| {{Main|Special relativity|Introduction to special relativity}}
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| [[Albert Einstein|Einstein's]] [[special relativity|theory of special relativity]], like Newtonian mechanics, assumes the equivalence of all inertial reference frames, but makes an additional assumption, foreign to Newtonian mechanics, namely, that in [[free space]] light always is propagated with the [[speed of light]] ''c''<sub>0</sub>, a defined [http://physics.nist.gov/cgi-bin/cuu/Value?c value] independent of its direction of propagation and its frequency, and also independent of the state of motion of the emitting body. This second assumption has been verified experimentally and leads to counter-intuitive deductions including:
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| * [[time dilation]] (moving clocks tick more slowly)
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| * [[length contraction]] (moving objects are shortened in the direction of motion)
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| * [[relativity of simultaneity]] (simultaneous events in one reference frame are not simultaneous in almost all frames moving relative to the first).
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| These deductions are [[logical consequence]]s of the stated assumptions, and are general properties of space-time, typically without regard to a consideration of properties pertaining to the structure of individual objects like atoms or stars, nor to the mechanisms of clocks.
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| These effects are expressed mathematically by the [[Lorentz transformation]]
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| :<math>x^{\prime} = \gamma \left(x - v t \right) </math>
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| :<math>y^{\prime} = y</math>
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| :<math>z^{\prime} = z</math>
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| :<math>t^{\prime} = \gamma \left(t - \frac{v x}{c_0^{2}}\right)</math>
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| where shifts in origin have been ignored, the relative velocity is assumed to be in the <math>x</math>-direction and the [[Lorentz factor]] γ is defined by:
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| :<math>
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| \gamma \ \stackrel{\mathrm{def}}{=}\
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| \frac{1}{\sqrt{1 - (v/c_0)^2}} \ \ge 1.
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| </math>
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| The Lorentz transformation is equivalent to the [[Galilean transformation]] in the limit ''c''<sub>0</sub> → ∞ (a hypothetical case) or ''v'' → 0 (low speeds).
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| Under [[Lorentz transformation]]s, the time and distance between events may differ among inertial reference frames; however, the [[Lorentz scalar]] distance ''s'' between two events is the same in all inertial reference frames
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| :<math>
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| s^{2} =
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| \left( x_{2} - x_{1} \right)^{2} + \left( y_{2} - y_{1} \right)^{2} +
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| \left( z_{2} - z_{1} \right)^{2} - c_0^{2} \left(t_{2} - t_{1}\right)^{2}
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| </math>
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| From this perspective, the [[speed of light]] is only accidentally a property of [[light]], and is rather a property of [[spacetime]], a [[conversion of units|conversion factor]] between conventional time units (such as [[second]]s) and length units (such as meters).
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| Incidentally, because of the limitations on speeds faster than the speed of light, notice that a rotating frame of reference (which is a non-inertial frame, of course) cannot be used out to arbitrary distances because at large radius its components would move faster than the speed of light.<ref name=Landau>{{Cite book|title=The Classical Theory of Fields |author=LD Landau & LM Lifshitz |edition=4th Revised English |pages=273–274 |year=1975 |isbn=978-0-7506-2768-9 |publisher=Pergamon Press }}</ref>
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| ==General relativity==
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| {{Main|General relativity|Introduction to general relativity}}
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| {{See also|Equivalence principle|Eötvös experiment}}
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| General relativity is based upon the principle of equivalence:<ref name=Morin>{{Cite book|title=Introduction to Classical Mechanics |author=David Morin |page=649 |url=http://books.google.com/?id=Ni6CD7K2X4MC&pg=PA469&dq=acceleration+azimuthal+inauthor:Morin |isbn=0-521-87622-2 |publisher=Cambridge University Press |year=2008}}</ref><ref name=Giancoli>{{Cite book|title=Physics for Scientists and Engineers with Modern Physics |author=Douglas C. Giancoli |url=http://books.google.com/?id=xz-UEdtRmzkC&pg=PA155&dq=%22principle+of+equivalence%22
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| |page=155 |year=2007 |publisher=Pearson Prentice Hall |isbn=0-13-149508-9 }}</ref>{{quote|There is no experiment observers can perform to distinguish whether an acceleration arises because of a gravitational force or because their reference frame is accelerating.|Douglas C. Giancoli, ''Physics for Scientists and Engineers with Modern Physics'', p. 155.}}
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| This idea was introduced in Einstein's 1907 article "Principle of Relativity and Gravitation" and later developed in 1911.<ref name=General_theory>A. Einstein, "On the influence of gravitation on the propagation of light", ''Annalen der Physik'', vol. 35, (1911) : 898-908</ref> Support for this principle is found in the [[Eötvös experiment]], which determines whether the ratio of inertial to gravitational mass is the same for all bodies, regardless of size or composition. To date no difference has been found to a few parts in 10<sup>11</sup>.<ref name=NRC>{{Cite book|title=Physics Through the Nineteen Nineties: Overview |page=15 |url=http://books.google.com/?id=Hk1wj61PlocC&pg=PA15&dq=equivalence+gravitation
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| |isbn=0-309-03579-1 |year=1986 |author=National Research Council (US) |publisher=National Academies Press }}</ref> For some discussion of the subtleties of the Eötvös experiment, such as the local mass distribution around the experimental site (including a quip about the mass of Eötvös himself), see Franklin.<ref name=Franklin>{{Cite book|title=No Easy Answers: Science and the Pursuit of Knowledge |author=Allan Franklin |page=66 |url=http://books.google.com/?id=_RN-v31rXuIC&pg=PA66&dq=%22Eotvos+experiment%22
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| |isbn=0-8229-5968-2 |year=2007 |publisher=University of Pittsburgh Press }}</ref>
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| Einstein’s [[general relativity|general theory]] modifies the distinction between nominally "inertial" and "noninertial" effects by replacing special relativity's "flat" [[Minkowski Space]] with a metric that produces non-zero curvature. In general relativity, the principle of inertia is replaced with the principle of [[geodesic (general relativity)|geodesic motion]], whereby objects move in a way dictated by the curvature of spacetime. As a consequence of this curvature, it is not a given in general relativity that inertial objects moving at a particular rate with respect to each other will continue to do so. This phenomenon of [[geodesic deviation]] means that inertial frames of reference do not exist globally as they do in Newtonian mechanics and special relativity.
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| However, the general theory reduces to the special theory over sufficiently small regions of spacetime, where curvature effects become less important and the earlier inertial frame arguments can come back into play.<ref>{{cite book |title=Information Theory and Quantum Physics: Physical Foundations for Understanding the Conscious Process |first1=Herbert S. |last1=Green |publisher=Springer |year=2000 |isbn=354066517X |page=154 |url=http://books.google.com/books?id=CUJiQjSVCu8C}}, [http://books.google.com/books?id=CUJiQjSVCu8C&pg=PA154 Extract of page 154] </ref><ref>{{cite book |title=Theory of Special Relativity |first1=Nikhilendu |last1=Bandyopadhyay |publisher=Academic Publishers |year=2000 |isbn=8186358528 |page=116 |url=http://books.google.com/books?id=qMOyfi_i0j8C}}, [http://books.google.com/books?id=qMOyfi_i0j8C&pg=PA116 Extract of page 116] </ref> Consequently, modern special relativity is now sometimes described as only a "local theory".<ref>{{cite book |title=Cosmological Inflation and Large-Scale Structure |first1=Andrew R. |last1=Liddle |first2=David H. |last2=Lyth |publisher=Cambridge University Press |year=2000 |isbn=0-521-57598-2 |page=329 |url=http://books.google.com/books?id=XmWauPZSovMC}}, [http://books.google.com/books?id=XmWauPZSovMC&pg=PA329 Extract of page 329] </ref>
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| ==See also==
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| {{Col-begin}}
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| {{Col-1-of-2}}
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| *[[Diffeomorphism]]
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| *[[Galilean invariance]]
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| *[[General covariance]]
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| {{Col-2-of-2}}
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| *[[Local reference frame]]
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| *[[Lorentz invariance]]
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| *[[Newton's laws of motion#Newton.27s first law|Newton's first law]]
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| {{col-end}}
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| ==References==
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| {{Reflist|2}}
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| ==Further reading==
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| * [[Edwin F. Taylor]] and [[John Archibald Wheeler]], ''Spacetime Physics'', 2nd ed. (Freeman, NY, 1992)
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| * [[Albert Einstein]], ''Relativity, the special and the general theories'', 15th ed. (1954)
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| * [[Henri Poincaré]], (1900) "La théorie de Lorentz et le Principe de Réaction", ''Archives Neerlandaises'', '''V''', 253–78.
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| * [[Albert Einstein]], ''On the Electrodynamics of Moving Bodies'', included in ''The Principle of Relativity'', page 38. Dover 1923
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| ;Rotation of the Universe
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| *{{Cite book|title=Mach's Principle: From Newton's Bucket to Quantum Gravity |page= 445 |author=Julian B. Barbour, Herbert Pfister |isbn=0-8176-3823-7 |year=1998 |url=http://books.google.com/?id=fKgQ9YpAcwMC&pg=PA445&dq=Birch++%22rotation+of+the+universe%22+-religion+-astrology+date:1990-2000 |publisher=Birkhäuser}}
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| *{{Cite book|title=Time Machines |author=PJ Nahin |page= 369; Footnote 12 |url=http://books.google.com/?id=39KQY1FnSfkC&pg=PA369 |year=1999 |isbn=0-387-98571-9 |publisher=Springer }}
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| *[http://www.nipne.ro/rjp/2008_53_1-2/0405_0416.pdf B Ciobanu, I Radinchi] ''Modeling the electric and magnetic fields in a rotating universe'' Rom. Journ. Phys., Vol. 53, Nos. 1–2, P. 405–415, Bucharest, 2008
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| *[http://arxiv.org/abs/gr-qc/0206080v1 Yuri N. Obukhov, Thoralf Chrobok, Mike Scherfner] ''Shear-free rotating inflation'' Phys. Rev. D 66, 043518 (2002) [5 pages]
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| *[http://arxiv.org/abs/astro-ph/0008106v1 Yuri N. Obukhov] ''On physical foundations and observational effects of cosmic rotation'' (2000)
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| *[http://arxiv.org/abs/astro-ph/9703082v1 Li-Xin Li] ''Effect of the Global Rotation of the Universe on the Formation of Galaxies'' General Relativity and Gravitation, '''30''' (1998) {{doi|10.1023/A:1018867011142}}
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| *[http://www.nature.com/nature/journal/v298/n5873/abs/298451a0.html P Birch] ''Is the Universe rotating?'' Nature 298, 451 - 454 (29 July 1982)
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| *[http://www.springerlink.com/content/t13ul36l27222351/fulltext.pdf?page=1 Kurt Gödel] ''An example of a new type of cosmological solutions of Einstein’s field equations of gravitation'' Rev. Mod. Phys., Vol. 21, p. 447, 1949.
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| ==External links==
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| * [http://plato.stanford.edu/entries/spacetime-iframes/ Stanford Encyclopedia of Philosophy entry]
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| * [http://www.youtube.com/watch?v=49JwbrXcPjc Animation clip] showing scenes as viewed from both an inertial frame and a rotating frame of reference, visualizing the Coriolis and centrifugal forces.
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| {{DEFAULTSORT:Inertial Frame Of Reference}}
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| [[Category:Classical mechanics]]
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| [[Category:Frames of reference]]
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| [[Category:Theory of relativity]]
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| [[Category:Orbits]]
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