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Abelardo M. Zerda III Michael O. Suarez Jm Dawn C. Rivas Leslie Kate Diane Berte.

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Presentation on theme: "Abelardo M. Zerda III Michael O. Suarez Jm Dawn C. Rivas Leslie Kate Diane Berte."— Presentation transcript:

1 Abelardo M. Zerda III Michael O. Suarez Jm Dawn C. Rivas Leslie Kate Diane Berte

2 Momentum and Impulse Conservation of Momentum Collisions in One Dimensions Collisions in Two Dimensions

3 Measure of one’s motion, equivalent to the product of one’s mass and velocity. Momentum involves motion and mass. Expressing the definition mathematically, p = mv where: p = momentum in kg-m/s units m = mass in kg units v = velocity of the object in m/s units

4 Calculate the momentum of a 100-kg missile traveling at 100 m/s eastward. A 100 kg car strikes a tree at 50 km/h. Find its momentum.

5 Impulse – force (F) applied by one object to another object within a given time interval Δt The formula to get impulse is: F Δt = Δp where: F Δt = impulse in N-s (newton-second) units Δp = change in momentum in kg-m/s units

6 A person in a sled with a total mass of 125 kg, slides down a grassy hill and reach a speed of 8 m/s at the bottom. If a pile of grass can exert a constant force of 250 newtons, how fast will the sled stop? A 100 kg car strikes a tree at 20 km/h and comes to a stop in 0.5 seconds. Find its initial momentum and the force on the car while it is being stopped.

7 In a collision, energy is not always conserved but all collisions have to conserve momentum if there is no net applied force. ∑ p before collision = ∑ p after collision

8 There are three types of collisions: 1.Elastic collisions – conserve kinetic energy 2.Inelastic collisions – do not conserve kinetic energy 3.Completely inelastic collision

9 Let us assume that for the two balls, one is running on a straight track toward the second one, which is stationary. Assume the following items are given: m 1 – mass of object 1 m 2 – mass of object 2 v 1 – velocity of object 1 before collision v 2 – velocity of object 2 before collision v 1 ’ – velocity of object 1 after collision v 2 ’ – velocity of object 2 after collision

10 Solving for the velocity of mass 1 after collision v 1 ’: v 1 ’ = [(m 1 – m 2 ) / (m 1 + m 2 )] v 1 Solving for the velocity of mass 2 after collision v 2 ’: v 2 ’ = [2m 1 / (m 1 + m 2 )] v 1

11 v 1 ’ = [(m 1 – m 2 ) / (m 1 + m 2 )] v 1 = [(m-m) / (m+m)] v 1 = 0 After colliding with m 2, m 1 stops. v 2 ’ = [2m 1 / (m 1 + m 2 )] v 1 = (2m / 2m) v 1 = v 1 Total energy transfer occurred between m 1 and m 2.

12 Since m 1 > m 2, the term (m 1 – m 2 ) is positive. v 1 ’ = [(m 1 – m 2 ) / (m 1 + m 2 )] v 1 m 1 still moves and v 1 ’ has the same direction as v 1. Since all the terms are nonzero then, v 2 ’ = [2m 1 / (m 1 + m 2 )] v 1 m 2 also moves and v 2 ’ has the same direction as v1

13 Since m 1 < m 2, the term (m 1 – m 2 ) is negative. v 1 ’ = [(m 1 – m 2 ) / (m 1 + m 2 )] v 1 m 1 still moves but in the opposite direction. v 2 ’ = [2m 1 / (m 1 + m 2 )] v 1 Since all the terms are nonzero, then m 2 also moves and v 2 has the same direction as v 1.

14 Inelastic collisions produce a combined mass after collision. The equation for this type of collision is: m 1 v 1 + m 2 v 2 = ( m 1 + m 2) v f where: m 1 + m 2 is the combined mass of the object V f is the final velocity value for the combined mass If m 2 v 2 = 0, v f = v 1 m 1/ ( m 1 + m 2)

15 Balanced momentum in the x-direction and y-direction Angles are arbitrary

16 Along the x-axis:  p x before collision =  p x after collision p 1 cos  1 + p 2 cos  2 = p 1 cos  1 + p 2 cos  2 Along the y-axis:  p y before collision =  p y after collision p 1 sin  1 + p 2 sin  2 = p 1 sin  1 + p 2 sin  2

17 A pool ball weighing 2 kg is traveling at 30  at 0.8 m/s hits another ball moving at 0.5 m/s at 180 . If the second ball leaves the collision at 0  and the first moves away at 150 , find the final velocity vectors of the balls.


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