ROTATIONAL AND TRANSLATIONAL QUANTITIES
Position
Velocity = d /dt = d/dt
Acceleration = d /dt = d/dt
Force = m =
Kinetic energy k = mv/2 k = I/2
Work W = W =
Power P = P =
Potential Energy U = -.d U = -.d
Momentum = m = or = I
Mass m Moment of inertia I = mr
Impulse = dt = = dt =
Thrust (dm/dt) (dI/dt)
For a constant acceleration only: For constant angular acceleration only:
r = vt + 0.5at = t + 0.5t
v = v + at = + t
v= v + 2ar = + 2
r = ( + v) (t/2) = (+ )(t/2)
For a system of particles with a CONSTANT total mass, M:
= M and = d/dt
= (r)/M and = M(d/dt).
For systems where the mass may or may not vary:
= d/dt = m(d/dt) + (dm/dt)
The second term is the linear thrust which acts like a force and produces an acceleration. A linear thrust exists if mass enters or leaves the system with a non- zero relative velocity. For a rocket, dm/dt is negative. The thrust of a rocket is in the negative or opposite direction of the exhaust velocity. A rocket will thrust up if mass is ejected down.
A force that acts for a finite time is called a linear impulse () which produces a finite change in the linear momentum. A torque that acts for a finite time is called an angular impulse () which produces a finite change in the angular momentum.
A torque is a force multiplied by a non-zero lever arm. The magnitude of a torque is:
Fl = Frsin
where r is a vector that starts at the pivot point and extends to where the force hits the body, is the angle between r and the force, and l = rsin is the lever arm or perpendicular distance of the force with respect to the pivot. For a rigid body, a body with a constant moment of inertia with respect to the pivot point,
= I
The general form for the angular momentum is:
=
For a constrained system or an object with a pivot axis through the center of mass which is a principle axis (axis of symmetry),
= I
Newton’s law for momentum applied to rotation is:
= d/dt
For = I,
= I(d/dt) + (dI/dt)
The second term is the angular thrust. An angular thrust exists if the moment of inertia (distribution of mass) is changing with a non-zero relative angular velocity about the pivot. The angular thrust acts like a torque and produces an angular acceleration.