See Euler-Lagrange equation on Wiktionary
{ "etymology_text": "Named after the Swiss mathematician and physicist Leonhard Euler (1707–1783), and the Italian-born French mathematician and astronomer Joseph Louis Lagrange (1736–1813).", "forms": [ { "form": "Euler-Lagrange equations", "tags": [ "plural" ] } ], "head_templates": [ { "args": {}, "expansion": "Euler-Lagrange equation (plural Euler-Lagrange equations)", "name": "en-noun" } ], "lang": "English", "lang_code": "en", "pos": "noun", "senses": [ { "categories": [ { "kind": "other", "name": "English entries with incorrect language header", "parents": [ "Entries with incorrect language header", "Entry maintenance" ], "source": "w" }, { "kind": "other", "name": "Pages with 1 entry", "parents": [], "source": "w" }, { "kind": "other", "name": "Pages with entries", "parents": [], "source": "w" }, { "kind": "topical", "langcode": "en", "name": "Mechanics", "orig": "en:Mechanics", "parents": [ "Physics", "Sciences", "All topics", "Fundamental" ], "source": "w" } ], "glosses": [ "A differential equation which describes a function mathbf q(t) which describes a stationary point of a functional, S( mathbf q)=∫L(t, mathbf q(t), mathbf ̇q(t)),dt, which represents the action of mathbf q(t), with L representing the Lagrangian. The said equation (found through the calculus of variations) is ∂L/∂ mathbf q=d/dt∂L/∂ mathbf ̇q and its solution for mathbf q(t) represents the trajectory of a particle or object, and such trajectory should satisfy the principle of least action." ], "id": "en-Euler-Lagrange_equation-en-noun-qKchPddK", "links": [ [ "mechanics", "mechanics" ], [ "differential equation", "differential equation" ], [ "function", "function" ], [ "functional", "functional" ], [ "action", "action" ], [ "Lagrangian", "Lagrangian" ], [ "calculus of variations", "calculus of variations" ], [ "trajectory", "trajectory" ], [ "principle of least action", "principle of least action" ] ], "qualifier": "analytical mechanics", "raw_glosses": [ "(mechanics, analytical mechanics) A differential equation which describes a function mathbf q(t) which describes a stationary point of a functional, S( mathbf q)=∫L(t, mathbf q(t), mathbf ̇q(t)),dt, which represents the action of mathbf q(t), with L representing the Lagrangian. The said equation (found through the calculus of variations) is ∂L/∂ mathbf q=d/dt∂L/∂ mathbf ̇q and its solution for mathbf q(t) represents the trajectory of a particle or object, and such trajectory should satisfy the principle of least action." ], "topics": [ "engineering", "mechanical-engineering", "mechanics", "natural-sciences", "physical-sciences" ], "wikipedia": [ "Euler-Lagrange equation", "Joseph Louis Lagrange", "Leonhard Euler" ] } ], "word": "Euler-Lagrange equation" }
{ "etymology_text": "Named after the Swiss mathematician and physicist Leonhard Euler (1707–1783), and the Italian-born French mathematician and astronomer Joseph Louis Lagrange (1736–1813).", "forms": [ { "form": "Euler-Lagrange equations", "tags": [ "plural" ] } ], "head_templates": [ { "args": {}, "expansion": "Euler-Lagrange equation (plural Euler-Lagrange equations)", "name": "en-noun" } ], "lang": "English", "lang_code": "en", "pos": "noun", "senses": [ { "categories": [ "English countable nouns", "English entries with incorrect language header", "English eponyms", "English lemmas", "English multiword terms", "English nouns", "Pages with 1 entry", "Pages with entries", "en:Mechanics" ], "glosses": [ "A differential equation which describes a function mathbf q(t) which describes a stationary point of a functional, S( mathbf q)=∫L(t, mathbf q(t), mathbf ̇q(t)),dt, which represents the action of mathbf q(t), with L representing the Lagrangian. The said equation (found through the calculus of variations) is ∂L/∂ mathbf q=d/dt∂L/∂ mathbf ̇q and its solution for mathbf q(t) represents the trajectory of a particle or object, and such trajectory should satisfy the principle of least action." ], "links": [ [ "mechanics", "mechanics" ], [ "differential equation", "differential equation" ], [ "function", "function" ], [ "functional", "functional" ], [ "action", "action" ], [ "Lagrangian", "Lagrangian" ], [ "calculus of variations", "calculus of variations" ], [ "trajectory", "trajectory" ], [ "principle of least action", "principle of least action" ] ], "qualifier": "analytical mechanics", "raw_glosses": [ "(mechanics, analytical mechanics) A differential equation which describes a function mathbf q(t) which describes a stationary point of a functional, S( mathbf q)=∫L(t, mathbf q(t), mathbf ̇q(t)),dt, which represents the action of mathbf q(t), with L representing the Lagrangian. The said equation (found through the calculus of variations) is ∂L/∂ mathbf q=d/dt∂L/∂ mathbf ̇q and its solution for mathbf q(t) represents the trajectory of a particle or object, and such trajectory should satisfy the principle of least action." ], "topics": [ "engineering", "mechanical-engineering", "mechanics", "natural-sciences", "physical-sciences" ], "wikipedia": [ "Euler-Lagrange equation", "Joseph Louis Lagrange", "Leonhard Euler" ] } ], "word": "Euler-Lagrange equation" }
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