the product of the magnitude of the force and the perpendicular distance etween the line of action of the force and the axis of rotation
translational equilibrium
the net force of the body is zero
rotational equilibrium
the net torque on the body is zero
moment of inertia
the distribution of mass of an extended body about an axis of rotation
angular momentum
the product of mass, speed and orbit radius of a particle
conservation of angular momentum
when the net torque on a system is zero, the angular momentum is conserved
angular impulse
the change in angular momentum
moment
its turning effect about a point
the product of the force and the perpendicular distance from the point of th eline of action of the force
the principle of moments
for a system of forces acting on an object to be in rotational equilibrium, the sum of the anti-clockwise moments about the same point
couple
a pair of equal sized forces that have different lines of action but which are parallel to each other and act in opposite directions, either side of the axis of rotation
a couple produces no resultant force on an object
there is no translation acceleration and the object remains in the same position in a couple
newton's second law for rotational motion
The resulting angular acceleration (α) of an object is directly proportional to the net torque (τ) on that object
conservation of angular momentum
the total angular momentum of a system is constant provided that no net external torque is acting on it
bodies in rotational equilibrium have a resultant torque of zero
unbalanced torque applied to an extended, rigid body will cause angular acceleration