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- 2. Outline Center of Mass Conservation of Linear Momentum Conservation of Angular Momentum Conservation of Energy Elastic Collision and Conservation Law Elastic Collision 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 2
- 9. 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 6
- 16. 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 13 Conservation of Linear Momentum : “the rate of change of total linear momentum is equal to the total external applied force” or In the term of center of mass coordinate system :
- 18. 3. Conservation of Angular Momentum 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 15 The angular momentum of a single particle is defined in terms of a cross product as : For N particles :
- 22. 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 18 Conservation of Angular Momentum : “For an isolated—one on which no net external forces act—the total torque τwill be zero; hence the angular momentum remains constant both in magnitude and direction”
- 23. 4. Conservation of Energy 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 19 In many situations, the total force acting on any particle in a system of particles is a function of the positions of the particles in the system : If the force Fksatisfies the condition that :
- 24. 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 20 There exists a potential function : Such that : The motion of kth particle is described by :
- 27. 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 24 Collisions may be divided into : elastic collisions inelastic collisions
- 32. 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 31