1. Ying Yi PhD Chapter 7 Impulse and Momentum 1 PHYS I @ HCC

2. Outline PHYS I @ HCC 2 Impulse and Momentum Theorem Conservation of Momentum Collision  Inelastic  Elastic

3. Momentum Definition: The linear momentum of an object of mass m moving with a velocity is defined as the product of the mass and the velocity SI Units: kgm / s Note that: Vector quantity, the direction of the momentum is the same as the velocity’s 3 PHYS I @ HCC

4. Components of Momentum X components: p x = m v x Y components: p y = m v y Momentum is related to kinetic energy 4 PHYS I @ HCC

5. Momentum and Kinetic Energy PHYS I @ HCC 5 Definition: Units: Relation: kgm / s J

6. Change of Momentum and Force In order to change the momentum of an object, a force must be applied The time rate of change of momentum of an object is equal to the net force acting on it Gives an alternative statement of Newton’s second law 6 PHYS I @ HCC

7. Impulse When a single, constant force acts on the object, there is an impulse delivered to the object is defined as the impulse Vector quantity, the direction is the same as the direction of the force 7 PHYS I @ HCC

8. Impulse-Momentum Theorem The theorem states that the impulse acting on the object is equal to the change in momentum of the object If the force is not constant, use the average force applied 8 PHYS I @ HCC

9. 9 Average Force in Impulse The average force can be thought of as the constant force that would give the same impulse to the object in the time interval as the actual time-varying force gives in the interval

10. Average Force cont. The impulse imparted by a force during the time interval Δ t is equal to the area under the force-time graph from the beginning to the end of the time interval Or, the impulse is equal to the average force multiplied by the time interval, 10 PHYS I @ HCC

11. Impulse Applied to Auto Collisions The most important factor is the collision time or the time it takes the person to come to a rest This will reduce the chance of dying in a car crash Ways to increase the time Seat belts Air bags 11 PHYS I @ HCC

12. 12 Typical Collision Values For a 75 kg person traveling at 27 m/s and coming to stop in 0.010 s F = -2.0 x 10 5 N a = 280 g Almost certainly fatal

13. Comparison of Accelerations PHYS I @ HCC 13 About 4g About 2g 280g

14. Survival Increase time Seat belt Restrain people so it takes more time for them to stop New time is about 0.15 seconds 14 PHYS I @ HCC

15. Air Bags The air bag increases the time of the collision It will also absorb some of the energy from the body It will spread out the area of contact Decreases the pressure Helps prevent penetration wounds 15 PHYS I @ HCC

16. Example 7.1 A well hit ball PHYS I @ HCC 16 A baseball (m=0.14 kg) has an initial velocity of V 0 =-38 m/s as it approaches a bat. We have chosen the direction of approach as the negative direction. The bat applies an average force F that is much larger that the weight of the ball, and the ball departs from the bat with a final velocity of V f =+58 m/s. (a) Determine the impulse applied to the ball by the bat. (b) Assuming that the time of the contact is ∆t=1.6×10 -3 s, find the average force exerted on the ball by the bat.

17. Group Problem: Teeing off PHYS I @ HCC 17 A golf ball with mass 5.0×10 -2 kg is struck with a club as in Figure 6.3. The force on the ball varies from zero when contact is made up to some maximum value and then back to zero when the ball leaves the club, as in the graph of force vs. time in Figure 6.1. Assume that the ball leaves the club face with a velocity of +44 m/s. (a) Find the magnitude of the impulse due to the collision. (b) Estimate the duration of the collision and the average force acting on the ball. (Assume contacting distance is 2cm.)

18. Conservation of Momentum PHYS I @ HCC 18 Newton’s Third Law

19. How about explosion? Momentum conserved? PHYS I @ HCC 19

20. Conservation of Momentum Momentum in an isolated system in which a collision occurs is conserved A collision may be the result of physical contact between two objects “Contact” may also arise from the electrostatic interactions of the electrons in the surface atoms of the bodies An isolated system will have no external forces 20 PHYS I @ HCC

21. Example 7.5 Assembling a Freight Train PHYS I @ HCC 21 A freight train is being assembled in a switching yard, and Figure 7.8 shows two boxcars. Car 1 has a mass of m 1 =65×10 3 kg and moves at a velocity of v 01 =+0.80 m/s. Car 2, with a mass of m 2 =92×103 kg and a velocity of v 02 =+1.3 m/s, overtakes car 1 and couples to it Neglecting friction, find the common velocity v f of the cars after they become coupled.

22. Group Problem: Ice Skaters PHYS I @ HCC 22 Starting from rest, two skaters push off against each other on smooth level ice, where friction is negligible. One is woman (m 1 =54 kg), and one is man (m 2 =88 kg). Part b of the drawing shows that the woman moves away with a velocity of v f1 =+2.5 m/s. Find the recoil velocity of v f2 of the man

23. Types of collisions PHYS I @ HCC 23 Inelastic Collision Elastic Collision Kinetic energy is not conserved. Some of the kinetic energy is converted into other types of energy such as heat, sound, work to permanently deform an object. Perfectly inelastic collisions occur when the objects stick together Both momentum and kinetic energy are conserved

24. Collision Examples PHYS I @ HCC 24

25. PHYS I @ HCC 25 Perfectly Inelastic Collisions When two objects stick together after the collision, they have undergone a perfectly inelastic collision Conservation of momentum becomes

26. Elastic Collisions Both momentum and kinetic energy are conserved Typically have two unknowns Solve the equations simultaneously 26 PHYS I @ HCC

27. Summary of Types of Collisions In an elastic collision, both momentum and kinetic energy are conserved In an inelastic collision, momentum is conserved but kinetic energy is not In a perfectly inelastic collision, momentum is conserved, kinetic energy is not, and the two objects stick together after the collision, so their final velocities are the same 27 PHYS I @ HCC

28. Problem Solving for One -Dimensional Collisions Coordinates: Set up a coordinate axis and define the velocities with respect to this axis Diagram: Draw all the velocity vectors and label the velocities and the masses Conservation of Momentum: Write a general expression for the total momentum of the system before and after the collision Conservation of Energy: If the collision is elastic, write a second equation for conservation of KE, or the alternative equation (perfectly elastic collisions) Solve: The resulting equations simultaneously 28 PHYS I @ HCC

29. Example 7.3 measuring the speed of a bullet PHYS I @ HCC 29 The ballistic pendulum shown in Figure 7.12 a consists of a stationary 2.5 kg block of wood suspended by a wire of negligible mass. A 0.0100 kg bullet is fired into the block, and the block (with the bullet in it) swings to a maximum height of 0.650 m above the initial position. Find the speed with which the bullet is fired. (Ignore air resistance)

30. Group Problem: A truck versus a compact PHYS I @ HCC 30 A pickup truck with mass 1.80×10 3 kg is traveling eastbound at +15.0 m/s, while a compact car with mass 9.00×10 2 kg is traveling west bound at -15.0 m/s. The vehicles collide head-on, becoming entangled. (a) Find the speed of the entangled vehicles after the collision. (b) Find the change in the velocity of each vehicle. (c) Find the change in the kinetic energy of the system consisting of both vehicles.

31. A collision in two dimensions For a general collision of two objects in three- dimensional space, the conservation of momentum principle implies that the total momentum of the system in each direction is conserved 31 PHYS I @ HCC

32. Problem Solving for Two-Dimensional Collisions Conservation of Momentum: Write expressions for the x and y components of the momentum of each object before and after the collision Write expressions for the total momentum before and after the collision in the x-direction and in the y-direction 32 PHYS I @ HCC

33. Group Problem: collision at an intersection PHYS I @ HCC 33 A car with mass 1.50×10 3 kg traveling east at a speed of 25.0 m/s collides at an intersection with a 2.50×10 3 kg van traveling north at a speed of 20.0 m/s. Find the magnitude and direction of the velocity of the wreckage after the collision, assuming that the vehicles undergo a perfectly inelastic collision and assuming that friction between the vehicles and the road can be neglected.

34. Thank you PHYS I @ HCC 34 Homework: 4,8,12,16,17,30,38,42,