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</h1> </div> </div> <div class="row"> <div class="col"> <div class="text-muted"> An Entity of Type: <a href="http://www.w3.org/2002/07/owl#Thing">Thing</a>, from Named Graph: <a href="http://dbpedia.org">http://dbpedia.org</a>, within Data Space: <a href="http://dbpedia.org">dbpedia.org</a> </div> </div> </div> <div class="row pt-2"> <div class="col-xs-9 col-sm-10"> In Newtonian mechanics, momentum (more specifically linear momentum or translational momentum) is the product of the mass and velocity of an object. It is a vector quantity, possessing a magnitude and a direction. If m is an object's mass and v is its velocity (also a vector quantity), then the object's momentum p is : In the International System of Units (SI), the unit of measurement of momentum is the kilogram metre per second (kg⋅m/s), which is equivalent to the newton-second. </div> <div class="col-xs-3 col-sm-2"> <a href="#" class="thumbnail"> <img src="http://commons.wikimedia.org/wiki/Special:FilePath/Billard.jpg?width=300" alt="thumbnail" class="img-fluid" /> </a> </div> </div> </div> </section>   <section> <div class="container-xl"> <div class="row"> <div class="table-responsive"> <table class="table table-hover table-sm table-light"> <thead> <tr> <th class="col-xs-3 ">Property</th> <th class="col-xs-9 px-3">Value</th> </tr> </thead> <tbody> <tr class="odd"><td class="col-2"><a class="uri" href="http://dbpedia.org/ontology/abstract">dbo:abstract</a> </td><td class="col-10 text-break"><ul> <li style="display:none;">الزخم، أو زخم الحركة أو كمية الحركة هو أحد الكميات الفيزيائية التي عرفت من خلال الفيزياء الكلاسيكية بأنها حاصل ضرب كتلة الجسم في سرعته، ينطبق على كمية الحركة أحد مبادئ الانحفاظ في الفيزياء الكلاسيكية وهو مبدأ حفظ الزخم أو قانون حفظ الزخم. ووحدات كمية الحركة أو زخم الحركة هي : كيلوجرام.متر/ثانية. (ar)</li> <li style="display:none;">Hybnost je fyzikální veličina, která je mírou posuvného pohybu tělesa a je součinem jeho hmotnosti a rychlosti. Hybnost ve své podstatě popisuje pohybový stav tělesa. Hybnost je vektorová veličina, stejně jako rychlost, a má stejný směr. Hybnost tělesa je rovná impulzu síly, který je potřeba na jeho uvedení z klidu do pohybu odpovídající rychlostí; na zastavení je potřeba impulz opačný. Hybnost je zachovávající se veličina. To znamená, že celková hybnost izolované soustavy se nemůže změnit, což je obsahem zákona zachování hybnosti. (cs)</li> <li style="display:none;">La quantitat de moviment o moment lineal (p) d'un cos és el producte de la seva massa per la seva velocitat mesurades en un determinat sistema de referència. Les seves unitats són kg·m·s-1 o, equivelentment, N·s. Es pot apreciar que un vaixell de gran tonatge pot tenir una gran quantitat de moviment encara que es mou a una velocitat petita, i pot ser igualat per una bala petita que surti a una gran velocitat.També, un objecte molt gran que es mou a una gran velocitat tindrà una enorme quantitat de moviment, com per exemple un camió baixant sense frens un pendent, però el mateix camió en repòs no tindrà cap quantitat de moviment. La definició matemàtica del moment lineal per un cos és: on p i v són vectorials i: p = moment linealm = massav = velocitat lineal Per un sistema de N partícules de massa i velocitat el total de la quantitat de moviment s'expressa com: i per a un sistema continu de masses es: Si es deriva p respecte al temps i suposant que la massa és constant, es troba el producte de la massa per l'acceleració que, segons la segona Llei de Newton, és igual a la força: on: F = forçam = massaa = acceleració lineal D'on es veu fàcilment que la força és igual a la variació del moment lineal respecte del temps. La mateixa relació en forma integral és: On es pot veure que una força sostinguda durant un llarg període produeix més canvi de quantitat de moviment que la mateixa força quan s'aplica un curt període.Així, per canviar la quantitat de moviment d'un objecte, importa tant la magnitud de la força com el temps d'actuació. Podrem definir l'impuls com el producte de la força per l'increment de temps. on F és la força aplicada i ∆t l'increment de temps. L'impuls canvia la quantitat de moviment de la mateixa manera que la força canvia la velocitat. Per la qual cosa, finalment, es defineix l'impuls rebut per un cos o partícula com la variació de la quantitat de moviment: on pf és la quantitat de moviment final i p0 la inicial. (ca)</li> <li style="display:none;">Στη Φυσική, η ορμή είναι μία φυσική ποσότητα που σχετίζεται με την ταχύτητα και τη μάζα ενός σώματος. (el)</li> <li style="display:none;">Der Impuls ist eine grundlegende physikalische Größe, die den mechanischen Bewegungszustand eines physikalischen Objekts charakterisiert. Der Impuls eines physikalischen Objekts ist umso größer, je schneller es sich bewegt und je größer seine Masse ist. Damit steht der Impuls für das, was in der Umgangssprache unscharf mit „Schwung“ und „Wucht“ bezeichnet wird. Das Formelzeichen des Impulses ist meist (von lateinisch pellere ‚stoßen, treiben‘). Die Einheit ist im Internationalen Einheitensystem [p] = 1 kg·m·s−1 = 1 N·s (Newton-Sekunde). Im Gegensatz zur kinetischen Energie ist der Impuls eine vektorielle Größe und hat damit einen Betrag und eine Richtung. Seine Richtung ist die Bewegungsrichtung des Objekts. Sein Betrag ist in der klassischen Mechanik durch das Produkt aus der Masse des Körpers und der Geschwindigkeit seines Massenmittelpunkts gegeben. In der relativistischen Mechanik gilt eine andere Formel (Viererimpuls), die für Geschwindigkeiten weit unterhalb der Lichtgeschwindigkeit näherungsweise mit der klassischen Formel übereinstimmt. Sie schreibt aber auch masselosen Objekten, die sich mit Lichtgeschwindigkeit bewegen, einen Impuls zu, z. B. klassischen elektromagnetischen Wellen oder Photonen. Der Impuls eines Körpers charakterisiert ausschließlich die Translationsbewegung seines Massenmittelpunkts. Eine eventuell zusätzlich vorhandene Rotation um den Massenmittelpunkt wird durch den Drehimpuls beschrieben. Der Impuls ist eine additive Größe. Der Gesamtimpuls eines Objekts mit mehreren Bestandteilen ist die Vektorsumme der Impulse seiner Teile. Der Impuls hängt, wie die Geschwindigkeit und die kinetische Energie, von der Wahl des Bezugssystems ab. In einem fest gewählten Inertialsystem ist der Impuls eine Erhaltungsgröße, das heißt: Ein Objekt, auf das von außen keine Kräfte wirken, behält seinen Gesamtimpuls nach Betrag und Richtung bei. Üben zwei Objekte wechselseitige Kräfte aufeinander aus, z. B. bei einem Stoßvorgang, ändern sich ihre beiden Impulse in entgegengesetzter Weise so, dass ihre vektorielle Summe erhalten bleibt. Die Größe, um die sich der Impuls für eines der Objekte ändert, wird als Impulsübertrag bezeichnet. Im Rahmen der klassischen Mechanik ist der Impulsübertrag unabhängig von der Wahl des Inertialsystems. Der Impulsbegriff entwickelte sich aus der Suche nach dem Maß für die in einem physikalischen Objekt vorhandene „Menge an Bewegung“, die aller Erfahrung nach bei allen inneren Prozessen erhalten bleibt. Daraus erklären sich die heute veralteten Bezeichnungen „Bewegungsgröße“ oder „Bewegungsmenge“ für den Impuls. Mit diesen Bezeichnungen konnte ursprünglich auch die kinetische Energie gemeint sein; erst Anfang des 19. Jahrhunderts wurden die Begriffe sauber unterschieden. Im Englischen wird der Impuls momentum genannt, während impulse den Impulsübertrag (Kraftstoß) bezeichnet. (de)</li> <li style="display:none;">En fiziko, movokvanto estas fizika kvanto rilatita al la rapido kaj la maso de objekto. Movokvanto estas la de translacia nevario. Tiel, eĉ kampoj samkiel aliaj aferoj, ne nur partikloj, povas havi movokvanton. Tamen, en kiu ne estas asimptote , movokvanto eĉ ne difiniĝas. (eo)</li> <li style="display:none;">Higidura-kantitatea, momentu lineala edo abiadura bateko masa eta abiaduraren arteko biderkadura da. Masa da da eta abiadura magnitude bektorial beraz, momentu lineala magnitude bektoriala da. Esan beharra dago, magnitude bektorial guztien moduan, momentu lineala erreferentzia-sistemaren menpe dagoela; hau da, behatzaile guztientzako gorputz baten abiadura berdina ez denez momentua ere ez da izango. Momentu ingeleseko momentum hitzetik eratorria da eta ez da nahastu behar "aldiune" kontzeptuarekin. (eu)</li> <li style="display:none;">En physique, la quantité de mouvement est le produit de la masse par le vecteur vitesse d'un corps matériel supposé ponctuel. Il s'agit donc d'une grandeur vectorielle, définie par , qui dépend du référentiel d'étude. Par additivité, il est possible de définir la quantité de mouvement d'un corps non ponctuel (ou système matériel), dont il est possible de démontrer qu'elle est égale à la quantité de mouvement de son centre d'inertie affecté de la masse totale du système, soit (C étant le centre d'inertie du système). La notion de quantité de mouvement s'introduit naturellement en dynamique : en fait, la relation fondamentale de la dynamique exprime le fait que l'action d'une force extérieure sur un système conduit à une variation de sa quantité de mouvement : . Par ailleurs elle fait partie, avec l'énergie, des grandeurs qui se conservent pour un système isolé, c'est-à-dire soumis à aucune action extérieure, ou si celles-ci sont négligeables ou se compensent. Cette propriété est utilisée notamment en théorie des collisions. En mécanique analytique ou quantique la quantité de mouvement apparaît naturellement comme la grandeur liée à l'invariance du hamiltonien ou du lagrangien dans une translation d'espace, c'est-à-dire à la propriété d'homogénéité de l'espace, qui est effectivement vérifiée en l'absence de forces ou champs extérieurs. Sur un plan plus général il s'agit en fait d'une des conséquences du théorème de Noether qui permet de relier symétrie continue d'un système et lois de conservation. La notion d'impulsion ou moment linéaire généralise en mécanique analytique celle de quantité de mouvement, en tant que moment conjugué des coordonnées cartésiennes , soit . Quantité de mouvement et impulsion sont souvent confondues en raison de leur coïncidence dans la majorité des cas. Néanmoins ces deux grandeurs sont distinctes. L'impulsion coïncide avec la quantité de mouvement lorsque les forces appliquées à la particule dérivent d'une énergie potentielle. L'analogue « angulaire » du moment linéaire est le moment angulaire généralement confondu avec le moment cinétique. Il est aussi possible de définir la quantité de mouvement, plus souvent alors appelée impulsion, pour le champ électromagnétique. Le plus souvent, il est fait référence à la densité volumique d'impulsion du champ donnée par . En mécanique relativiste, les notions de quantité de mouvement et d'énergie sont liées par l'introduction du quadrivecteur énergie-impulsion , où γ est le facteur de Lorentz. En mécanique quantique, la quantité de mouvement est définie comme un « opérateur vectoriel », c'est-à-dire comme un ensemble de trois opérateurs (un par composante spatiale) qui respectent certaines relations de commutation (dites canoniques) avec les composantes de l'opérateur de position. (fr)</li> <li style="display:none;">La cantidad de movimiento, momento lineal, ímpetu, momentum o simplemente momento, es una magnitud física derivada de tipo vectorial que describe el movimiento de un cuerpo en cualquier teoría mecánica. En mecánica clásica, la cantidad de movimiento se define como el producto de la masa del cuerpo y su velocidad en un instante determinado. Históricamente, el concepto se remonta a Galileo Galilei. En su obra Discursos y demostraciones matemáticas en torno a dos nuevas ciencias, usa el término italiano impeto, mientras que Isaac Newton en Principia Mathematica usa el término latino motus (movimiento) y vis motrix (fuerza motriz). La definición concreta de cantidad de movimiento difiere de una formulación mecánica a otra: en mecánica newtoniana se define para una partícula simplemente como el producto de su masa por la velocidad, en la mecánica lagrangiana o hamiltoniana se admiten formas más complicadas en sistemas de coordenadas no cartesianas, en la teoría de la relatividad la definición es más compleja aun cuando se usan sistemas inerciales, y en mecánica cuántica su definición requiere el uso de operadores autoadjuntos definidos sobre un espacio vectorial de dimensión infinita. En mecánica newtoniana, la forma más usual de introducir la cantidad de movimiento es como el producto de la masa (kg) de un cuerpo material por su velocidad (m/s), para luego analizar su relación con las leyes de Newton. No obstante, tras el desarrollo de la física moderna, esta manera de operar no resultó ser la más conveniente para abordar esta magnitud derivada. Una diferencia importante es que esta definición newtoniana solo se tiene en cuenta el concepto inherente a la magnitud, que resulta ser una propiedad de cualquier ente físico con o sin masa, necesaria para describir las interacciones. Los modelos actuales consideran que no solo los cuerpos másicos poseen cantidad de movimiento, también resulta ser un atributo de los campos y los fotones. La cantidad de movimiento obedece a una ley de conservación, lo cual significa que la cantidad de movimiento total de todo sistema cerrado (o sea uno que no es afectado por fuerzas exteriores, y cuyas fuerzas internas no son disipadoras) no puede ser cambiada y permanece constante en el tiempo. En el enfoque geométrico de la mecánica relativista la definición es algo diferente. Además, el concepto de momento lineal puede definirse para entidades físicas como los fotones o los campos electromagnéticos, que carecen de masa en reposo. (es)</li> <li>In Newtonian mechanics, momentum (more specifically linear momentum or translational momentum) is the product of the mass and velocity of an object. It is a vector quantity, possessing a magnitude and a direction. If m is an object's mass and v is its velocity (also a vector quantity), then the object's momentum p is : In the International System of Units (SI), the unit of measurement of momentum is the kilogram metre per second (kg⋅m/s), which is equivalent to the newton-second. Newton's second law of motion states that the rate of change of a body's momentum is equal to the net force acting on it. Momentum depends on the frame of reference, but in any inertial frame it is a conserved quantity, meaning that if a closed system is not affected by external forces, its total linear momentum does not change. Momentum is also conserved in special relativity (with a modified formula) and, in a modified form, in electrodynamics, quantum mechanics, quantum field theory, and general relativity. It is an expression of one of the fundamental symmetries of space and time: translational symmetry. Advanced formulations of classical mechanics, Lagrangian and Hamiltonian mechanics, allow one to choose coordinate systems that incorporate symmetries and constraints. In these systems the conserved quantity is generalized momentum, and in general this is different from the kinetic momentum defined above. The concept of generalized momentum is carried over into quantum mechanics, where it becomes an operator on a wave function. The momentum and position operators are related by the Heisenberg uncertainty principle. In continuous systems such as electromagnetic fields, fluid dynamics and deformable bodies, a momentum density can be defined, and a continuum version of the conservation of momentum leads to equations such as the Navier–Stokes equations for fluids or the Cauchy momentum equation for deformable solids or fluids. (en)</li> <li style="display:none;">Sa bhfisic, iolrú an luais is na maise. Úsáidtear an tsiombail p chuige. Is é an dara dlí gluaiseachta de chuid Newton gurb ionann an fórsa agus ráta athraithe an mhóimintim in aghaidh an ama. Is prionsabal bunúsach sa bhfisic é, má tá córas ann nach bhfuil aon fhórsa i bhfeidhm air, go n-imchoimeádtar an móiminteam ann. Is cianníocht veicteoireach é. (ga)</li> <li style="display:none;">Dalam fisika, momentum atau pusa adalah besaran yang berhubungan dengan kecepatan dan massa suatu benda. (in)</li> <li style="display:none;">( 모멘텀은 여기로 연결됩니다. 다른 뜻에 대해서는 모멘텀 (동음이의) 문서를 참고하십시오.) 운동량 (運動量, 영어: momentum)은 물리학 특히, 뉴턴 역학에서 물체의 질량과 속도의 곱으로 나타내는 물리량이다. 운동량의 국제 단위는 뉴턴 초 (N · s) 또는 킬로그램 미터 매 초 (kg · m/s)이고, 통상적인 기호는 라틴 소문자 p이다. 선형 운동량(linear momentum) 혹은 병진 운동량(translational momentum)이라고도 부른다. 예를 들어 빠르게 움직이는 무거운 트럭 같은 물체는 운동량이 크다. 무거운 트럭을 빠른 속도까지 가속시키기 위해서는 큰 힘을 한참 동안 가해야 하고, 반대로 그 트럭을 정지시키기 위해서도 큰 힘을 오랫동안 가해야 한다. 트럭이 더 가볍다거나 더 느리게 움직인다면 그만큼 운동량도 작아질 것이다. 선형 운동량은 보존되는 양으로, 외부에서 가해지는 힘에 의한 영향이 없는 닫힌계의 선형 운동량의 총합은 바뀌지 않는다. 고전역학에서는 선형 운동량 보존법칙이 뉴턴의 운동 법칙에 포함되어 있다. 하지만 특수 상대성 이론에서도 공식을 약간 수정한 형태로 선형 운동량 보존 법칙을 충족시킬 수 있으며, (일반화된) 선형 운동량 보존 법칙은 적절한 정의를 이용하면 전자기학, 양자역학, 양자장론, 일반 상대성 이론에도 적용할 수 있는 보존 법칙이다. (ko)</li> <li style="display:none;">Pęd – wektorowa wielkość fizyczna opisująca mechanikę, a więc ruch i oddziaływania obiektu fizycznego. Pęd mogą mieć wszystkie formy materii, np. ciała o niezerowej masie spoczynkowej, pole elektromagnetyczne, pole grawitacyjne. (pl)</li> <li style="display:none;">In meccanica classica, la quantità di moto di un oggetto è una grandezza vettoriale definita come il prodotto della massa dell'oggetto per la sua velocità. Talvolta il vettore quantità di moto viene denominato momento lineare, per distinguerlo dal momento angolare. Tuttavia, a rigore questa quantità non rappresenta il momento di alcun vettore.Generalmente viene indicato con la lettera p o con la lettera q. Il secondo principio della dinamica stabilisce che la derivata temporale della quantità di moto di un corpo è eguale alla forza agente. La quantità di moto dipende dal sistema di riferimento, ma in un qualsiasi sistema di riferimento inerziale è una grandezza fisica conservativa, questo significa chese ho un sistema chiuso non soggetto a forze esterne, la quantità di moto non cambia nel tempo. La quantità di motosi conserva anche in relatività ristretta ma l'espressione matematica è diversa, come anche è diversa la formulazione in elettromagnetismo, meccanica quantistica, teoria quantistica dei campi e in relatività generale. La conservazione della quantità di moto dipende dalla omogeneità dello spazio ovvero dalla simmetria traslazionale. Nella formulazione della meccanica lagrangiana è possibile scegliere un sistema di coordinate che unisce simmetrie e vincoli. In questa formulazione la grandezza conservata è la quantità di moto generalizzata che in generale è diversa dalla quantità di moto definita prima.Il concetto di momento generalizzato viene importato in meccanica quantistica, in cui diviene un operatore che agisce sulla funzione d'onda. Gli operatori quantità di moto e posizione sono legati tra loro dal principio di indeterminazione di Heisenberg. Nei mezzi continui come sono i campi elettromagnetici, la dinamica dei fluidi e i corpi deformabilisi definisce la densità di quantità di moto. La formulazione nel continuo della legge di conservazione della quantità di moto diviene una equazione differenziale e, ad esempio, per i fluidi si hal'equazione di Navier–Stokes. (it)</li> <li style="display:none;">In de natuurkunde is de impuls of hoeveelheid van beweging (in het Engels momentum, niet te verwarren met het Engelse impulse (stoot)) een grootheid die gerelateerd is aan de snelheid en de massa van een object. Binnen de klassieke mechanica is impuls gedefinieerd als: , dus als het product van de scalaire grootheid massa en de vectoriële grootheid snelheid. De impuls is dus ook een vectorgrootheid, met dezelfde richting als de snelheid. De eenheid van impuls is (newtonseconde), wat in SI-eenheden neerkomt op . (nl)</li> <li style="display:none;">運動量（うんどうりょう、（英: momentum）とは、初等的には物体の運動の状態を表す物理量で、質量と速度の積として定義される。この意味の運動量は後述する一般化された運動量と区別して、運動学的運動量（あるいは動的運動量）と呼ばれる。また、角運動量という運動量とは異なる量と対比する上で、線型運動量などと呼ばれることもある。 (ja)</li> <li style="display:none;">Em ciência, momento linear refere-se a uma das duas grandezas físicas necessárias à correta descrição do inter-relacionamento - sempre mútuo - entre dois ou sistemas físicos. A segunda grandeza é a energia. Os entes ou sistemas em interação trocam energia e momento, mas o fazem de forma que ambas as grandezas sempre obedeçam à respectiva lei de conservação. A energia é uma grandeza escalar que tem por grandeza conjugada o tempo; ao passo que o momento é uma grandeza vetorial que tem por grandeza conjugada o vetor posição. Um ente físico é essencialmente caracterizado pela sua relação de dispersão, a relação entre energia e momento para o ente. (pt)</li> <li style="display:none;">Inom klassisk mekanik, definieras rörelsemängden (SI-enhet kg·m/s) som produkten av ett objekts massa och hastighet. I allmänhet kan rörelsemängden uppfattas som ett mått på hur svårt det är att ändra ett objekts rörelsetillstånd, bestämt av två faktorer: dess massa och dess hastighet. Detta kan ses som en naturlig konsekvens av Newtons första lag och Newtons andra lag. Reducerad hastighet eller massa resulterar i mindre rörelsemängd och omvänt. Rörelsemängd är en bevarad storhet i den betydelsen att den totala rörelsemängden för ett slutet system (ett som inte påverkas av yttre krafter) inte kan ändras. (sv)</li> <li style="display:none;">И́мпульс (коли́чество движе́ния) — векторная физическая величина, являющаяся мерой механического движения тела. В классической механике импульс тела равен произведению массы этого тела на его скорость направление импульса совпадает с направлением вектора скорости: В релятивистской физике импульс вычисляется как: где — скорость света; в пределе для малых формула переходит в классическую. Важнейший физический закон в котором фигурирует импульс тела, — второй закон Ньютона: здесь — время, — сила, приложенная к телу. В записи через импульс (в отличие от — ускорение) закон применим не только в классической, но и в релятивистской механике. В самом общем виде, определение звучит: импульс — это аддитивный интеграл движения механической системы, связанный согласно теореме Нётер с фундаментальной симметрией — однородностью пространства. Понятие «импульс» имеет обобщения в теоретической механике, для случая наличия электромагнитного поля (как для частицы в поле, так и для самого поля), а также в квантовой механике. (ru)</li> <li style="display:none;">Імпульсом або вектором кількості руху в класичній механіці називається міра механічного руху тіла, векторна величина, що для матеріальної точки дорівнює добутку маси точки на її швидкість та має напрямок швидкості. У Міжнародній системі одиниць (SI) одиницею імпульсу є кг·м/с, в системі СГС — [г·см/с]. Сума векторів імпульсу тіл для будь-якої ізольованої системи є величиною сталою. (uk)</li> <li style="display:none;">在古典力学裏，动量（momentum，p）被量化为物体的质量和速度的乘積（）。例如，一輛快速移動的重型卡車擁有很大的動量。若要使這重型卡車從零速度加速到移動速度，則需要使到很大的作用力；若要使重型卡車從移動速度減速到零，則也需要使到很大的作用力；若卡車輕一點或移動速度慢一點，則它的動量也會小一點。动量在国际单位制中的单位为kg·m/s。有關动量的更精确的量度的内容，请参见本页的部分。一般而言，一个物体的动量指的是这个物体在它运动方向上保持运动的趋势。动量实际上是牛顿第一定律的一个推论。动量是个向量，其方向与速度方向相同。动量同时也是一个守恒量，这表示为在一个封闭系统内动量的总和不可改变。在经典力学中，动量守恒暗含在牛顿定律中，但在狭义相对论中依然成立，（广义）动量在电动力学、量子力学、量子场论、广义相对论中也成立。勒内·笛卡儿认为宇宙中总的“运动的量”是保持守恒的，这里所说的“运动的量”被理解为“物体大小和速度的乘积”——但这不宜被解读为现代动量定律的表达方式，因为笛卡尔并没有把“质量”这个概念与物体“重量”和“大小”之间的关系区分开来，更重要的是他认为速率（标量）而不是速度（向量）是守恒的。因此对于笛卡兒来说：一个移动的物体从另一个表面弹回来的时候，该物体的方向发生了改变但速率没有发生改变，运动的量应该没有发生改变。 (zh)</li> </ul></td></tr><tr class="even"><td class="col-2"><a class="uri" href="http://dbpedia.org/ontology/thumbnail">dbo:thumbnail</a> </td><td class="col-10 text-break"><ul> <li><a class="uri" rel="dbo:thumbnail" resource="http://commons.wikimedia.org/wiki/Special:FilePath/Billard.jpg?width=300" 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prefix="dcterms: http://purl.org/dc/terms/" href="http://dbpedia.org/resource/Category:Motion_(physics)">dbc:Motion_(physics)</a></li> <li><a class="uri" rel="dcterms:subject" resource="http://dbpedia.org/resource/Category:Vector_physical_quantities" prefix="dcterms: http://purl.org/dc/terms/" href="http://dbpedia.org/resource/Category:Vector_physical_quantities">dbc:Vector_physical_quantities</a></li> </ul></td></tr><tr class="odd"><td class="col-2"><a class="uri" href="http://www.w3.org/1999/02/22-rdf-syntax-ns#type">rdf:type</a> </td><td class="col-10 text-break"><ul> <li><a class="uri" rel="rdf:type" resource="http://www.w3.org/2002/07/owl#Thing" href="http://www.w3.org/2002/07/owl#Thing">owl:Thing</a></li> </ul></td></tr><tr class="even"><td class="col-2"><a class="uri" href="http://www.w3.org/2000/01/rdf-schema#comment">rdfs:comment</a> </td><td class="col-10 text-break"><ul> <li style="display:none;">الزخم، أو زخم الحركة أو كمية الحركة هو أحد الكميات الفيزيائية التي عرفت من خلال الفيزياء الكلاسيكية بأنها حاصل ضرب كتلة الجسم في سرعته، ينطبق على كمية الحركة أحد مبادئ الانحفاظ في الفيزياء الكلاسيكية وهو مبدأ حفظ الزخم أو قانون حفظ الزخم. ووحدات كمية الحركة أو زخم الحركة هي : كيلوجرام.متر/ثانية. (ar)</li> <li style="display:none;">Hybnost je fyzikální veličina, která je mírou posuvného pohybu tělesa a je součinem jeho hmotnosti a rychlosti. Hybnost ve své podstatě popisuje pohybový stav tělesa. Hybnost je vektorová veličina, stejně jako rychlost, a má stejný směr. Hybnost tělesa je rovná impulzu síly, který je potřeba na jeho uvedení z klidu do pohybu odpovídající rychlostí; na zastavení je potřeba impulz opačný. Hybnost je zachovávající se veličina. To znamená, že celková hybnost izolované soustavy se nemůže změnit, což je obsahem zákona zachování hybnosti. (cs)</li> <li style="display:none;">Στη Φυσική, η ορμή είναι μία φυσική ποσότητα που σχετίζεται με την ταχύτητα και τη μάζα ενός σώματος. (el)</li> <li style="display:none;">En fiziko, movokvanto estas fizika kvanto rilatita al la rapido kaj la maso de objekto. Movokvanto estas la de translacia nevario. Tiel, eĉ kampoj samkiel aliaj aferoj, ne nur partikloj, povas havi movokvanton. Tamen, en kiu ne estas asimptote , movokvanto eĉ ne difiniĝas. (eo)</li> <li style="display:none;">Higidura-kantitatea, momentu lineala edo abiadura bateko masa eta abiaduraren arteko biderkadura da. Masa da da eta abiadura magnitude bektorial beraz, momentu lineala magnitude bektoriala da. Esan beharra dago, magnitude bektorial guztien moduan, momentu lineala erreferentzia-sistemaren menpe dagoela; hau da, behatzaile guztientzako gorputz baten abiadura berdina ez denez momentua ere ez da izango. Momentu ingeleseko momentum hitzetik eratorria da eta ez da nahastu behar "aldiune" kontzeptuarekin. (eu)</li> <li style="display:none;">Sa bhfisic, iolrú an luais is na maise. Úsáidtear an tsiombail p chuige. Is é an dara dlí gluaiseachta de chuid Newton gurb ionann an fórsa agus ráta athraithe an mhóimintim in aghaidh an ama. Is prionsabal bunúsach sa bhfisic é, má tá córas ann nach bhfuil aon fhórsa i bhfeidhm air, go n-imchoimeádtar an móiminteam ann. Is cianníocht veicteoireach é. (ga)</li> <li style="display:none;">Dalam fisika, momentum atau pusa adalah besaran yang berhubungan dengan kecepatan dan massa suatu benda. (in)</li> <li style="display:none;">Pęd – wektorowa wielkość fizyczna opisująca mechanikę, a więc ruch i oddziaływania obiektu fizycznego. Pęd mogą mieć wszystkie formy materii, np. ciała o niezerowej masie spoczynkowej, pole elektromagnetyczne, pole grawitacyjne. (pl)</li> <li style="display:none;">In de natuurkunde is de impuls of hoeveelheid van beweging (in het Engels momentum, niet te verwarren met het Engelse impulse (stoot)) een grootheid die gerelateerd is aan de snelheid en de massa van een object. Binnen de klassieke mechanica is impuls gedefinieerd als: , dus als het product van de scalaire grootheid massa en de vectoriële grootheid snelheid. De impuls is dus ook een vectorgrootheid, met dezelfde richting als de snelheid. De eenheid van impuls is (newtonseconde), wat in SI-eenheden neerkomt op . (nl)</li> <li style="display:none;">運動量（うんどうりょう、（英: momentum）とは、初等的には物体の運動の状態を表す物理量で、質量と速度の積として定義される。この意味の運動量は後述する一般化された運動量と区別して、運動学的運動量（あるいは動的運動量）と呼ばれる。また、角運動量という運動量とは異なる量と対比する上で、線型運動量などと呼ばれることもある。 (ja)</li> <li style="display:none;">Em ciência, momento linear refere-se a uma das duas grandezas físicas necessárias à correta descrição do inter-relacionamento - sempre mútuo - entre dois ou sistemas físicos. A segunda grandeza é a energia. Os entes ou sistemas em interação trocam energia e momento, mas o fazem de forma que ambas as grandezas sempre obedeçam à respectiva lei de conservação. A energia é uma grandeza escalar que tem por grandeza conjugada o tempo; ao passo que o momento é uma grandeza vetorial que tem por grandeza conjugada o vetor posição. Um ente físico é essencialmente caracterizado pela sua relação de dispersão, a relação entre energia e momento para o ente. (pt)</li> <li style="display:none;">Імпульсом або вектором кількості руху в класичній механіці називається міра механічного руху тіла, векторна величина, що для матеріальної точки дорівнює добутку маси точки на її швидкість та має напрямок швидкості. У Міжнародній системі одиниць (SI) одиницею імпульсу є кг·м/с, в системі СГС — [г·см/с]. Сума векторів імпульсу тіл для будь-якої ізольованої системи є величиною сталою. (uk)</li> <li style="display:none;">在古典力学裏，动量（momentum，p）被量化为物体的质量和速度的乘積（）。例如，一輛快速移動的重型卡車擁有很大的動量。若要使這重型卡車從零速度加速到移動速度，則需要使到很大的作用力；若要使重型卡車從移動速度減速到零，則也需要使到很大的作用力；若卡車輕一點或移動速度慢一點，則它的動量也會小一點。动量在国际单位制中的单位为kg·m/s。有關动量的更精确的量度的内容，请参见本页的部分。一般而言，一个物体的动量指的是这个物体在它运动方向上保持运动的趋势。动量实际上是牛顿第一定律的一个推论。动量是个向量，其方向与速度方向相同。动量同时也是一个守恒量，这表示为在一个封闭系统内动量的总和不可改变。在经典力学中，动量守恒暗含在牛顿定律中，但在狭义相对论中依然成立，（广义）动量在电动力学、量子力学、量子场论、广义相对论中也成立。勒内·笛卡儿认为宇宙中总的“运动的量”是保持守恒的，这里所说的“运动的量”被理解为“物体大小和速度的乘积”——但这不宜被解读为现代动量定律的表达方式，因为笛卡尔并没有把“质量”这个概念与物体“重量”和“大小”之间的关系区分开来，更重要的是他认为速率（标量）而不是速度（向量）是守恒的。因此对于笛卡兒来说：一个移动的物体从另一个表面弹回来的时候，该物体的方向发生了改变但速率没有发生改变，运动的量应该没有发生改变。 (zh)</li> <li style="display:none;">La quantitat de moviment o moment lineal (p) d'un cos és el producte de la seva massa per la seva velocitat mesurades en un determinat sistema de referència. Les seves unitats són kg·m·s-1 o, equivelentment, N·s. La definició matemàtica del moment lineal per un cos és: on p i v són vectorials i: p = moment linealm = massav = velocitat lineal Per un sistema de N partícules de massa i velocitat el total de la quantitat de moviment s'expressa com: i per a un sistema continu de masses es: on: F = forçam = massaa = acceleració lineal La mateixa relació en forma integral és: (ca)</li> <li style="display:none;">Der Impuls ist eine grundlegende physikalische Größe, die den mechanischen Bewegungszustand eines physikalischen Objekts charakterisiert. Der Impuls eines physikalischen Objekts ist umso größer, je schneller es sich bewegt und je größer seine Masse ist. Damit steht der Impuls für das, was in der Umgangssprache unscharf mit „Schwung“ und „Wucht“ bezeichnet wird. Das Formelzeichen des Impulses ist meist (von lateinisch pellere ‚stoßen, treiben‘). Die Einheit ist im Internationalen Einheitensystem [p] = 1 kg·m·s−1 = 1 N·s (Newton-Sekunde). (de)</li> <li style="display:none;">La cantidad de movimiento, momento lineal, ímpetu, momentum o simplemente momento, es una magnitud física derivada de tipo vectorial que describe el movimiento de un cuerpo en cualquier teoría mecánica. En mecánica clásica, la cantidad de movimiento se define como el producto de la masa del cuerpo y su velocidad en un instante determinado. Históricamente, el concepto se remonta a Galileo Galilei. En su obra Discursos y demostraciones matemáticas en torno a dos nuevas ciencias, usa el término italiano impeto, mientras que Isaac Newton en Principia Mathematica usa el término latino motus (movimiento) y vis motrix (fuerza motriz). (es)</li> <li>In Newtonian mechanics, momentum (more specifically linear momentum or translational momentum) is the product of the mass and velocity of an object. It is a vector quantity, possessing a magnitude and a direction. If m is an object's mass and v is its velocity (also a vector quantity), then the object's momentum p is : In the International System of Units (SI), the unit of measurement of momentum is the kilogram metre per second (kg⋅m/s), which is equivalent to the newton-second. (en)</li> <li style="display:none;">En physique, la quantité de mouvement est le produit de la masse par le vecteur vitesse d'un corps matériel supposé ponctuel. Il s'agit donc d'une grandeur vectorielle, définie par , qui dépend du référentiel d'étude. Par additivité, il est possible de définir la quantité de mouvement d'un corps non ponctuel (ou système matériel), dont il est possible de démontrer qu'elle est égale à la quantité de mouvement de son centre d'inertie affecté de la masse totale du système, soit (C étant le centre d'inertie du système). (fr)</li> <li style="display:none;">In meccanica classica, la quantità di moto di un oggetto è una grandezza vettoriale definita come il prodotto della massa dell'oggetto per la sua velocità. Talvolta il vettore quantità di moto viene denominato momento lineare, per distinguerlo dal momento angolare. Tuttavia, a rigore questa quantità non rappresenta il momento di alcun vettore.Generalmente viene indicato con la lettera p o con la lettera q. (it)</li> <li style="display:none;">( 모멘텀은 여기로 연결됩니다. 다른 뜻에 대해서는 모멘텀 (동음이의) 문서를 참고하십시오.) 운동량 (運動量, 영어: momentum)은 물리학 특히, 뉴턴 역학에서 물체의 질량과 속도의 곱으로 나타내는 물리량이다. 운동량의 국제 단위는 뉴턴 초 (N · s) 또는 킬로그램 미터 매 초 (kg · m/s)이고, 통상적인 기호는 라틴 소문자 p이다. 선형 운동량(linear momentum) 혹은 병진 운동량(translational momentum)이라고도 부른다. 예를 들어 빠르게 움직이는 무거운 트럭 같은 물체는 운동량이 크다. 무거운 트럭을 빠른 속도까지 가속시키기 위해서는 큰 힘을 한참 동안 가해야 하고, 반대로 그 트럭을 정지시키기 위해서도 큰 힘을 오랫동안 가해야 한다. 트럭이 더 가볍다거나 더 느리게 움직인다면 그만큼 운동량도 작아질 것이다. (ko)</li> <li style="display:none;">Inom klassisk mekanik, definieras rörelsemängden (SI-enhet kg·m/s) som produkten av ett objekts massa och hastighet. I allmänhet kan rörelsemängden uppfattas som ett mått på hur svårt det är att ändra ett objekts rörelsetillstånd, bestämt av två faktorer: dess massa och dess hastighet. Detta kan ses som en naturlig konsekvens av Newtons första lag och Newtons andra lag. Reducerad hastighet eller massa resulterar i mindre rörelsemängd och omvänt. (sv)</li> <li style="display:none;">И́мпульс (коли́чество движе́ния) — векторная физическая величина, являющаяся мерой механического движения тела. В классической механике импульс тела равен произведению массы этого тела на его скорость направление импульса совпадает с направлением вектора скорости: В релятивистской физике импульс вычисляется как: где — скорость света; в пределе для малых формула переходит в классическую. Важнейший физический закон в котором фигурирует импульс тела, — второй закон Ньютона: здесь — время, — сила, приложенная к телу. (ru)</li> </ul></td></tr><tr class="odd"><td class="col-2"><a class="uri" href="http://www.w3.org/2000/01/rdf-schema#label">rdfs:label</a> </td><td class="col-10 text-break"><ul> <li>Momentum (en)</li> <li style="display:none;">زخم الحركة (ar)</li> <li style="display:none;">Quantitat de moviment (ca)</li> <li style="display:none;">Hybnost (cs)</li> <li style="display:none;">Impuls (de)</li> <li style="display:none;">Ορμή (el)</li> <li style="display:none;">Movokvanto (eo)</li> <li style="display:none;">Cantidad de movimiento (es)</li> <li style="display:none;">Momentu lineal (eu)</li> <li style="display:none;">Móiminteam (ga)</li> <li style="display:none;">Momentum (in)</li> <li style="display:none;">Quantità di moto (it)</li> <li style="display:none;">Quantité de mouvement (fr)</li> <li style="display:none;">運動量 (ja)</li> <li style="display:none;">운동량 (ko)</li> <li style="display:none;">Impuls (natuurkunde) (nl)</li> <li style="display:none;">Pęd (fizyka) (pl)</li> <li style="display:none;">Momento linear (pt)</li> <li style="display:none;">Импульс (ru)</li> <li style="display:none;">Rörelsemängd (sv)</li> <li style="display:none;">动量 (zh)</li> <li style="display:none;">Імпульс (механіка) (uk)</li> </ul></td></tr><tr class="even"><td class="col-2"><a class="uri" href="http://www.w3.org/2000/01/rdf-schema#seeAlso">rdfs:seeAlso</a> </td><td class="col-10 text-break"><ul> <li><a class="uri" rel="rdfs:seeAlso" resource="http://dbpedia.org/resource/Analytical_mechanics" href="http://dbpedia.org/resource/Analytical_mechanics">dbr:Analytical_mechanics</a></li> <li><a class="uri" rel="rdfs:seeAlso" resource="http://dbpedia.org/resource/Mass" href="http://dbpedia.org/resource/Mass">dbr:Mass</a></li> <li><a class="uri" rel="rdfs:seeAlso" resource="http://dbpedia.org/resource/Variable-mass_system" href="http://dbpedia.org/resource/Variable-mass_system">dbr:Variable-mass_system</a></li> <li><a class="uri" rel="rdfs:seeAlso" 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