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Sesion #25-28 MekanikaKlasik Riser Fahdiran, M.Si Umiatin, M.Si JurusanFisika FakultasMatematikadanIlmuPengetahuanAlam
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
System of Particles 05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 3
The Aim : 05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 4 ,[object Object]
Understanding of conservations law are required to explore those motion
Two approach are used :
Newton’s Law
Symmetry principles,[object Object]
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 6
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 7 ,[object Object],[object Object]
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 9 ,[object Object],	There are 3N simultaneous second order differential equation to be solved, with 6N arbitrary constant ( 3N for initial position and 3N for initial velocity) Alternative Method : 	by using the center of mass coordinates
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 10 ,[object Object]
Or :
For N particles :,[object Object]
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 12 ,[object Object],	According to Newton's third law, the force exerted on the kthparticle due to the /th particle is equal and opposite to that exerted on l by k : 	The sum of internal force , the right side contains forces on all pairs of particles:
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 :
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 14 ,[object Object],	The center of mass of a system of particles moves like a single particle of mass M (total mass of the system) acted on by a single force F that is equal to the sum of all the external forces acting on the system.
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 :
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 16 ,[object Object]
The first term on the right vanishes because :
The second term is equal to the total force acting on the particle k,= 0,[object Object]
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”
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 :
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 :
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 21 ,[object Object]
Where :,[object Object],[object Object]
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 24 	Collisions may be divided into :  elastic collisions inelastic collisions
6. Elastic Collision 05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 25
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 26 ,[object Object]
After simple operation finally we find :,[object Object],[object Object],[object Object]
05/01/2011 ©  2010 Universitas Negeri Jakarta   |  www.unj.ac.id                      | 30 ,[object Object],	The two particles leave at right angles to each other. The example of such a collision is observed on a pool table when a cue ball is seen to leave the struck ball at a right angle.

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Mekanika Klasik (25 - 28)

  • 1. Sesion #25-28 MekanikaKlasik Riser Fahdiran, M.Si Umiatin, M.Si JurusanFisika FakultasMatematikadanIlmuPengetahuanAlam
  • 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
  • 3. System of Particles 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 3
  • 4.
  • 5. Understanding of conservations law are required to explore those motion
  • 8.
  • 9. 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 6
  • 10.
  • 11.
  • 12.
  • 13. Or :
  • 14.
  • 15.
  • 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 :
  • 17.
  • 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 :
  • 19.
  • 20. The first term on the right vanishes because :
  • 21.
  • 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 :
  • 25.
  • 26.
  • 27. 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 24 Collisions may be divided into : elastic collisions inelastic collisions
  • 28. 6. Elastic Collision 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 25
  • 29.
  • 30.
  • 31.
  • 32. 05/01/2011 © 2010 Universitas Negeri Jakarta | www.unj.ac.id | 31