Angular Momentum of a Particle

The angular momentum of a particle of mass m with respect to a chosen origin is given by 一个质量为m的质点相对于所选原点的角动量由 L = mvr sin θ or more formally by the vector product 或更正式地说，通过矢量积 L = r x p The direction is given by the right hand rule which would give L the direction out of the diagram. For an orbit, angular momentum is conserved, and this leads to one of Kepler's laws. For a circular orbit, L becomes 方向由右手法则给出，这会使L指向图外。对于轨道，角动量是守恒的，这导致了开普勒定律之一。对于圆轨道，L变为 L = mvr L = mvr sin θ L = r × p L = mvr

Angular Momentum

The angular momentum of a rigid object is defined as the product of the moment of inertia and the angular velocity. It is analogous to linear momentum and is subject to the fundamental constraints of the conservation of angular momentum principle if there is no external torque on the object. Angular momentum is a vector quantity. It is derivable from the expression for the angular momentum of a particle

Angular and Linear Momentum

Angular momentum and linear momentum are examples of the parallels between linear and rotational motion. They have the same form and are subject to the fundamental constraints of conservation laws, the conservation of momentum and the conservation of angular momentum .