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Force
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{{Short description|Influence that can change motion of an object}} {{Redirect|Physical force||Force (disambiguation)|and|Physical force (disambiguation)}} {{Infobox physical quantity | name = Force | width = | background = | image = [[File:Force examples.svg|200px]] | caption = Forces can be described as a push or pull on an object. They can be due to phenomena such as [[gravity]], [[magnetism]], or anything that might cause a mass to accelerate. | unit = [[newton (unit)|newton]] (N) | otherunits = [[dyne]], [[pound-force]], [[poundal]], [[kip (unit)|kip]], [[kilopond]] | symbols = <math>\vec F</math>, {{mvar|F}}, {{math|'''F'''}} | baseunits = [[kilogram|kg]]Β·[[metre|m]]Β·[[second|s]]<sup>β2</sup> | dimension = wikidata | derivations = {{math|1='''F''' = ''[[Mass|m]]''[[Acceleration|'''a''']]}} }} {{Classical mechanics|expanded=Fundamental concepts}} In [[physics]], a '''force''' is an influence that can cause an [[Physical object|object]] to change its [[velocity]] unless counterbalanced by other forces. In mechanics, force makes ideas like ''''pushing'''' or ''''pulling'''' mathematically precise. Because the [[Magnitude (mathematics)|magnitude]] and [[Direction (geometry, geography)|direction]] of a force are both important, force is a [[Euclidean vector|vector]] quantity. The [[SI unit]] of force is the [[newton (unit)|newton (N)]], and force is often represented by the symbol {{math|'''F'''}}. Force plays an important role in classical mechanics. The concept of force is central to all three of [[Newton's laws of motion]]. Types of forces often encountered in [[classical mechanics]] include [[Elasticity (physics)|elastic]], [[friction]]al, [[Normal force|contact or "normal" forces]], and [[gravity|gravitational]]. The rotational version of force is [[torque]], which produces [[angular acceleration|changes in the rotational speed]] of an object. In an extended body, each part applies forces on the adjacent parts; the distribution of such forces through the body is the internal [[stress (mechanics)|mechanical stress]]. In the case of multiple forces, if the net force on an extended body is zero the body is in equilibrium. In [[modern physics]], which includes [[Theory of relativity|relativity]] and [[quantum mechanics]], the laws governing motion are revised to rely on [[fundamental interactions]] as the ultimate origin of force. However, the understanding of force provided by classical mechanics is useful for practical purposes.<ref>{{Cite web |last=Cohen |first=Michael |title=Classical Mechanics: a Critical Introduction |url=https://www.physics.upenn.edu/sites/default/files/Classical_Mechanics_a_Critical_Introduction_0_0.pdf |url-status=live |archive-url=https://web.archive.org/web/20220703194458/https://www.physics.upenn.edu/sites/default/files/Classical_Mechanics_a_Critical_Introduction_0_0.pdf |archive-date=July 3, 2022 |access-date=January 9, 2024 |website=[[University of Pennsylvania]]}}</ref>
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