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Lecture no 17&18 Conservation of Momentum

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Presentation on theme: "Lecture no 17&18 Conservation of Momentum"— Presentation transcript:

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2 Lecture no 17&18 Conservation of Momentum
Prepared by Engr.Sarfaraz Khan Turk Lecturer at IBT LUMHS Jamshoro

3 Momentum In classical mechanics, linear momentum or translational momentum (pl. momenta; SI unit kg m/s, or equivalently, N s) is the product of the mass and velocity of an object. For example, a heavy truck moving fast has a large momentum—it takes a large and prolonged force to get the truck up to this speed, and it takes a large and prolonged force to bring it to a stop afterwards. If the truck were lighter, or moving more slowly, then it would have less momentum. Like velocity, linear momentum is a vector quantity, possessing a direction as well as a magnitude:p=mv

4 Momentum Linear momentum is also a conserved quantity, meaning that if a closed system is not affected by external forces, its total linear momentum cannot change. In classical mechanics, conservation of linear momentum is implied by Newton's laws; but it also holds in special relativity (with a modified formula) and, with appropriate definitions, a (generalized) linear momentum conservation law holds in electrodynamics, quantum mechanics, quantum field theory, and general relativity.

5 Conservation of Momentum

6 Conservation on Momentum
In the absence of an external force the momentum of a closed system is conserved.

7 Law of Conservation of Momentum
In a closed system, the vector sum of the momenta before and after an impact must be equal. Before After m1v1 +m2v2 = m1v1’ + m2v2’

8 Closed System: A system that has no gain nor loss of mass.

9 Isolated System: A closed system with no net external force acting on it.

10 Internal and External Forces
Internal Forces: act between objects within a system. External Forces: are exerted by objects outside the system.

11 A stationary firecracker explodes
A stationary firecracker explodes. What is the total momentum of the pieces that it breaks into? Question Coyle ,4th of July 2009, Hudson River

12 Example: Recoiling Cannon

13 Example 1: Recoiling Cannon
A cannon of mass 750kg shoots a cannon ball of mass 30kg with a velocity of 20m/s. Find the recoil velocity of the cannon. m1v1 +m2v = m1v1’ + m2v2’ Answer: -0.8m/s

14 Collisions Elastic (Kinetic Energy is conserved)
Inelastic (Kinetic Energy is not conserved) Deformed objects Objects stick together Note: Momentum is conserved in both types of collisions.

15 Example 2: Inelastic Collision
A bullet of mass 0.010kg is shot at a speed of 30m/s towards a 5kg stationary block. The bullet becomes embedded in the block an the two fly off together. Find the speed with which they fly off. Answer: 0.06m/s

16 Problem 3 A 45 kg student is riding on a 7kg scateboard with a velocity of +4m/s. The student jumps of the cart with a velocity of -1m/s. Find the velocity of the scateboard after the student jumped off. Answer: +36m/s


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