[{"@context":"http:\/\/schema.org\/","@type":"BlogPosting","@id":"https:\/\/wiki.edu.vn\/en\/wiki14\/gravitational-field-wikipedia\/#BlogPosting","mainEntityOfPage":"https:\/\/wiki.edu.vn\/en\/wiki14\/gravitational-field-wikipedia\/","headline":"Gravitational field – Wikipedia","name":"Gravitational field – Wikipedia","description":"before-content-x4 Model in physics “Gravity field” redirects here. For Earth’s gravity field, see Gravity of Earth. after-content-x4 In physics, a","datePublished":"2017-09-25","dateModified":"2017-09-25","author":{"@type":"Person","@id":"https:\/\/wiki.edu.vn\/en\/wiki14\/author\/lordneo\/#Person","name":"lordneo","url":"https:\/\/wiki.edu.vn\/en\/wiki14\/author\/lordneo\/","image":{"@type":"ImageObject","@id":"https:\/\/secure.gravatar.com\/avatar\/44a4cee54c4c053e967fe3e7d054edd4?s=96&d=mm&r=g","url":"https:\/\/secure.gravatar.com\/avatar\/44a4cee54c4c053e967fe3e7d054edd4?s=96&d=mm&r=g","height":96,"width":96}},"publisher":{"@type":"Organization","name":"Enzyklop\u00e4die","logo":{"@type":"ImageObject","@id":"https:\/\/wiki.edu.vn\/wiki4\/wp-content\/uploads\/2023\/08\/download.jpg","url":"https:\/\/wiki.edu.vn\/wiki4\/wp-content\/uploads\/2023\/08\/download.jpg","width":600,"height":60}},"image":{"@type":"ImageObject","@id":"https:\/\/wikimedia.org\/api\/rest_v1\/media\/math\/render\/svg\/893605d8e9a94d69baf6aa04b7437f8d0257b399","url":"https:\/\/wikimedia.org\/api\/rest_v1\/media\/math\/render\/svg\/893605d8e9a94d69baf6aa04b7437f8d0257b399","height":"","width":""},"url":"https:\/\/wiki.edu.vn\/en\/wiki14\/gravitational-field-wikipedia\/","wordCount":4091,"articleBody":"     (adsbygoogle = window.adsbygoogle || []).push({});before-content-x4Model in physics“Gravity field” redirects here. For Earth’s gravity field, see Gravity of Earth.       (adsbygoogle = window.adsbygoogle || []).push({});after-content-x4In physics, a gravitational field is a model used to explain the influences that a massive body extends into the space around itself, producing a force on another massive body.[1] Thus, a gravitational field is used to explain gravitational phenomena, and is measured in newtons per kilogram (N\/kg).  Equivalently, it is measured in meters per second squared (m\/s2).In its original concept, gravity was a force between point masses. Following Isaac Newton, Pierre-Simon Laplace attempted to model gravity as some kind of radiation field or fluid, and since the 19th century, explanations for gravity have usually been taught in terms of a field model, rather than a point attraction.In a field model, rather than two particles attracting each other, the particles distort spacetime via their mass, and this distortion is what is perceived and measured as a “force”.[citation needed]    In such a model one states that matter moves in certain ways in response to the curvature of spacetime,[2] and that there is either no gravitational force,[3] or that gravity is a fictitious force.[4]       (adsbygoogle = window.adsbygoogle || []).push({});after-content-x4Gravity is distinguished from other forces by its obedience to the equivalence principle.Classical mechanics[edit]In classical mechanics, a gravitational field is a physical quantity.[5] A gravitational field can be defined using Newton’s law of universal gravitation. Determined in this way, the gravitational field g around a single particle of mass M is a vector field consisting at every point of a vector pointing directly towards the particle. The magnitude of the field at every point is calculated by applying the universal law, and represents the force per unit mass on any object at that point in space. Because the force field is conservative, there is a scalar potential energy per unit mass, \u03a6, at each point in space associated with the force fields; this is called gravitational potential.[6] The gravitational field equation is[7]g=Fm=d2Rdt2=\u2212GMR^|R|2=\u2212\u2207\u03a6{displaystyle mathbf {g} ={frac {mathbf {F} }{m}}={frac {d^{2}mathbf {R} }{dt^{2}}}=-GM{frac {mathbf {hat {R}} }{left|mathbf {R} right|^{2}}}=-nabla Phi }where F is the gravitational force, m is the mass of the test particle, R is the position of the test particle (or for Newton’s second law of motion which is a time dependent function, a set of positions of test particles each occupying a particular point in space for the start of testing), R\u0302 is a unit vector in the radial direction of R, t is time, G is the gravitational constant, and \u2207 is the del operator.       (adsbygoogle = window.adsbygoogle || []).push({});after-content-x4This includes Newton’s law of universal gravitation, and the relation between gravitational potential and field acceleration. Note that d2R\/dt2 and F\/m are both equal to the gravitational acceleration g (equivalent to the inertial acceleration, so same mathematical form, but also defined as gravitational force per unit mass[8]). The negative signs are inserted since the force acts antiparallel to the displacement. The equivalent field equation in terms of mass density \u03c1 of the attracting mass is:\u2207\u22c5g=\u2212\u22072\u03a6=\u22124\u03c0G\u03c1{displaystyle nabla cdot mathbf {g} =-nabla ^{2}Phi =-4pi Grho }which contains Gauss’s law for gravity, and Poisson’s equation for gravity. Newton’s law implies Gauss’s law, but not vice versa; see Relation between Gauss’s and Newton’s laws.These classical equations are differential equations of motion for a test particle in the presence of a gravitational field, i.e. setting up and solving these equations allows the motion of a test mass to be determined and described.The field around multiple particles is simply the vector sum of the fields around each individual particle. An object in such a field will experience a force that equals the vector sum of the forces it would experience in these individual fields. This is mathematically[9]gj(net)=\u2211i\u2260jgi=1mj\u2211i\u2260jFi=\u2212G\u2211i\u2260jmiR^ij|Ri\u2212Rj|2=\u2212\u2211i\u2260j\u2207\u03a6i{displaystyle mathbf {g} _{j}^{text{(net)}}=sum _{ineq j}mathbf {g} _{i}={frac {1}{m_{j}}}sum _{ineq j}mathbf {F} _{i}=-Gsum _{ineq j}m_{i}{frac {mathbf {hat {R}} _{ij}}{left|mathbf {R} _{i}-mathbf {R} _{j}right|^{2}}}=-sum _{ineq j}nabla Phi _{i}}i.e. the gravitational field on mass mj is the sum of all gravitational fields due to all other masses mi, except the mass mj itself. The unit vector R\u0302ij is in the direction of Rj \u2212 Ri (pointing from particle i to particle j).General relativity[edit]In general relativity, the Christoffel symbols play the role of the gravitational force field and the metric tensor plays the role of the gravitational potential.In general relativity, the gravitational field is determined by solving the Einstein field equations[10]G=\u03baT,{displaystyle mathbf {G} =kappa mathbf {T} ,}where T is the stress\u2013energy tensor, G is the Einstein tensor, and \u03ba is the Einstein gravitational constant.  The latter is defined as \u03ba = 8\u03c0G\/c4, where G is the Newtonian constant of gravitation and c is the speed of light.These equations are dependent on the distribution of matter and energy in a region of space, unlike Newtonian gravity, which is dependent only on the distribution of matter.  The fields themselves in general relativity represent the curvature of spacetime.  General relativity states that being in a region of curved space is equivalent to accelerating up the gradient of the field.  By Newton’s second law, this will cause an object to experience a fictitious force if it is held still with respect to the field.  This is why a person will feel himself pulled down by the force of gravity while standing still on the Earth’s surface.  In general the gravitational fields predicted by general relativity differ in their effects only slightly from those predicted by classical mechanics, but there are a number of easily verifiable differences, one of the most well known being the deflection of light in such fields.See also[edit]^ Feynman, Richard (1970). The Feynman Lectures on Physics. Vol.\u00a0I. Addison Wesley Longman. ISBN\u00a0978-0-201-02115-8.^ Geroch, Robert (1981). General Relativity from A to B. University of Chicago Press. p.\u00a0181. ISBN\u00a0978-0-226-28864-2.^ Gr\u00f8n, \u00d8yvind; Hervik, Sigbj\u00f8rn (2007). Einstein’s General Theory of Relativity: with Modern Applications in Cosmology. Springer Japan. p.\u00a0256. ISBN\u00a0978-0-387-69199-2.^ Foster, J.; Nightingale, J. D. (2006). A Short Course in General Relativity (3\u00a0ed.). Springer Science & Business. p.\u00a055. ISBN\u00a0978-0-387-26078-5.^ Feynman, Richard (1970). The Feynman Lectures on Physics. Vol.\u00a0II. Addison Wesley Longman. ISBN\u00a0978-0-201-02115-8. A “field” is any physical quantity which takes on different values at different points in space.^ Forshaw, J. R.; Smith, A. G. (2009). Dynamics and Relativity. Wiley. ISBN\u00a0978-0-470-01460-8.[page\u00a0needed]^ Lerner, R. G.; Trigg, G. L., eds. (1991). Encyclopaedia of Physics (2nd\u00a0ed.). Wiley-VCH. ISBN\u00a0978-0-89573-752-6.[page\u00a0needed]^ Whelan, P. M.; Hodgeson, M. J. (1978). Essential Principles of Physics (2nd\u00a0ed.). John Murray. ISBN\u00a0978-0-7195-3382-2.[page\u00a0needed]^ Kibble, T. W. B. (1973). Classical Mechanics. European Physics Series (2nd\u00a0ed.). UK: McGraw Hill. ISBN\u00a0978-0-07-084018-8.[page\u00a0needed]^ Wheeler, J. A.; Misner, C.; Thorne, K. S. (1973). Gravitation. W. H. Freeman & Co. p.\u00a0404. ISBN\u00a0978-0-7167-0344-0.     (adsbygoogle = window.adsbygoogle || []).push({});after-content-x4"},{"@context":"http:\/\/schema.org\/","@type":"BreadcrumbList","itemListElement":[{"@type":"ListItem","position":1,"item":{"@id":"https:\/\/wiki.edu.vn\/en\/wiki14\/#breadcrumbitem","name":"Enzyklop\u00e4die"}},{"@type":"ListItem","position":2,"item":{"@id":"https:\/\/wiki.edu.vn\/en\/wiki14\/gravitational-field-wikipedia\/#breadcrumbitem","name":"Gravitational field – Wikipedia"}}]}]