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Material Type: Notes; Professor: Bombelli; Class: Physics for Science & Engineering I; Subject: Physics; University: University of Mississippi Main Campus; Term: Fall 2009;
Typology: Study notes
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Chapter 11: Rolling, Torque, and Angular Momentum Rolling: If the object does not slip, its linear and angular motions are related by s = R and v com
and the kinetic energy is K = I P^2 = I com^2 + mv^2. Problem solving: Be able to set up and solve problems with rolling objects using Newton's second law and/or conservation of energy. Angular momentum: For a particle moving in space, the angular momentum with respect to a point is l = r x p. For a system of particles, the total angular momentum L is the sum (as a vector) of all the l 's. For an object rotating around a fixed axis, the important component is the components along that axis, which is L = I , where I is the rotational inertia around that axis. Rotational inertia: For a small object of mass m a distance r away from the rotation axis, I = mr 2 . Torque: For a particle or other object moving in space, the torque of a force F with respect to a point is = r x F , where r is the radius vector from the reference point to the point where F is applied. Angular form of second law: The net torque (^) net = d L /d t is the time derivative of the angular momentum. Conservation of angular momentum: If the net (external) torque on a system is zero, its angular momentum L is conserved, L i = L f. Precession of a gyroscope: We only saw a demonstration of precession – it will not be on tests. Website by Luca Bombelli <bombelli"at"olemiss.edu>; Content of this page last modified on 8 nov 2009