Total linear momentum: P=Ĭonservation Theorem for the Linear Momentum of a System of Particles: If the total external force is zero, the total linear momentum is conserved. Internal forces that obey Newton’s third law, have no effect on the motion of the center of mass. R= M mi Center of mass moves as if the total external force were acting on the entire mass of the system concentrated at the center of mass. It is called the weak law of action and reaction. Newton’s third law of motion, equal and opposite forces, does not hold for all forces. The Conservation Theorem for the Angular Momentum of a Particle states that angular momentum, L, is conserved if the total torque T, is zero. The Conservation Theorem for the Linear Momentum of a Particle states that linear momentum, p, is conserved if the total force F, is zero. Energy Conservation Theorem for a Particle: If forces acting on a particle are conservative, then the total energy of the particle, T + V, is conserved. To express work in a way that is independent of the path taken, a change in a quantity that depends on only the end points is needed. The capacity to do work that a body or system has by viture of is position is called its potential energy. dr = 0 If friction is present, a system is non-conservative.Independence of W12 on the particular path implies that the work done around a closed ciruit is zero: I F T =Ī force is considered conservative if the work is the same for any physically possible path. Mv 2 2 The work is the change in kinetic energy. dv W12 = m dt 1 dt 1 1 m W12 = (v22 − v12 ) = T2 − T1 2 Kinetic Energy: Z.In most cases, mass is constant and work simplifies to: 2 Torque is the time derivative of angular momentum: dt2 Newton’s second law of motion holds in a reference frame that is inertial or Galilean. dt In most cases, mass is constant and force is simplified: F=Īcceleration: d2 r. ‘Classical’ refers to the contradistinction to ‘quantum’ mechanics. Goldstein Classical Mechanics Notes Michael Good May 30, 2004Ĭlassical mechanics incorporates special relativity.
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