The relativistic version of this quantity is represented as a second-order antisymmetric tensor, while its kinetic, gauge-invariant variety is determined by r cross quantity P minus electric charge times A close quantity. The specific relative flavor of this quantity is always perpendicular to the instantaneous osculating (OS-kyuh-lay-ting) orbital plane and a relation based on this quantity can be used to explain the Law of (*) Areas, as it is an application where mass is held constant. The presence of this quantity explains why an already-spun bicycle wheel attached to a rope will precess about the axis of the rope after it is released, and it is often incorrectly believed only to exist in systems undergoing obvious rotation. For 10 point
The relativistic version of this quantity is represented as a second-order antisymmetric tensor, while its kinetic, gauge-invariant variety is determined by r cross quantity P minus electric charge times A close quantity. The specific relative flavor of this quantity is always perpendicular to the instantaneous osculating (OS-kyuh-lay-ting) orbital plane and a relation based on this quantity can be used to explain the Law of (*) Areas, as it is an application where mass is held constant. The presence of this quantity explains why an already-spun bicycle wheel attached to a rope will precess about the axis of the rope after it is released, and it is often incorrectly believed only to exist in systems undergoing obvious rotation. For 10 points, name this physical property, denoted by L, which is conserved in systems unless they are subject to external torque.
The relativistic version of this quantity is represented as a second-order antisymmetric tensor, while its kinetic, gauge-invariant variety is determined by r cross quantity P minus electric charge times A close quantity.
angular momentum [accept L before mention]