t 1 + u 1-2 = t 2 conservation of energy principle of work and energy

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T 1 + U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

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Page 1: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

T1 + U1-2 = T2

Conservation of Energy

Principle of Work and Energy

Page 2: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

CHAPTER 15

Kinetics of a Particle: Impulse and Momentum

Page 3: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Objectives

1. To develop the principle of linear impulse and momentum for a particle

2. To study the conservation of linear momentum for a particle

3. To analyze the mechanics of impact

Page 4: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

T1 + U1-2 = T2

Principle of Work and Energy

v = ds/dta = dv/dt

dt = ds/vdt = dv/a

ads = vdv

Page 5: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

a = dv/dtads = vdv

Principle of Linear Impulse and Momentum

Page 6: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Linear Impulse

Variable Force Constant Force

Page 7: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

+ =

Page 8: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Principle of Linear Impulse and Momentum

a particle

system of particles

Page 9: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

100 kg stone is originally at rest on the smooth horizontal space.If a towing force of 200 N, acting at an angle of 45o, is appliedto the stone for 10 s, determine the final velocity and the normal forcewhich the surface exerts on the stone during the time interval.

ex1

Page 10: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Principle of Impulse and momentum

+

Page 11: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Principle of Impulse and momentum

+

Page 12: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

The 250 N crate is acted upon by a force having a variable magnitude P = 100t, where t is in seconds. Determine the crate’s velocity 2 s afterP has been applied. The initial velocity is v1 = 1 m/s down the plane,and k = 0.3.

Page 13: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Principle of Linear Impulse and Momentum

a particle

system of particles

Page 14: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Conservation of Linear Momentum for a System of Particles

When the sum of the external impulses acting on a system of a particleis zero,

Nonimpulsive force : - impulse that may be neglected - considered equal to zero

Impulsive : - forces that are very large and act for a very short period of time

produce significant change in momentum

Page 15: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

The force of the rackets on the ball is impulsiveThe ball’s weight will have the negligible effect, nonimpulsive

Page 16: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Boxcar A : 15 MgBoxcar B : 12 Mg

Ex1

If the car meets and couple together, determine(a) the speed of both cars just after the coupling(b) the average force between them if the coupling takes place in 0.8 s

Page 17: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Conservation of Linear Momentum

(a) the speed of both cars just after the coupling

Page 18: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Principles of Impulse and Momentum

(b) the average force between them if the coupling takes place in 0.8 s

Page 19: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

The 600 kg cannon shown fires a 4 kg projectile with a muzzle velocity450 m/s relative to the ground. If firing takes place in 0.03 s, determine

(a) the recoil velocity of the cannon just after firing(b) the average impulsive force acting on the projectile

The cannon support is fixed to the ground, and the horizontal recoil of the cannon is absorbed by two springs.

Ex 2

Page 20: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Conservation of Linear Momentum

Mc = 600 [kg]Mp = 4 [kg](Vp )1 = 450 [m/s]t = 0.03 [s]

Page 21: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Priciples of Impulse and Momentum

Page 22: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Lab test 2 : 12/04/07 (Khamis)

Mid-Term 2 : 16/04/07 (Isnin)

Page 23: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Objectives

1. To develop the principle of linear impulse and momentum for a particle

2. To study the conservation of linear momentum for a particle

3. To analyze the mechanics of impact

Page 24: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Impact

Impact occurs when two bodies collide with each other during a veryshort period of time, causing relatively large (impulsive ) forces to beexerted between the bodies.

Page 25: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Central Impact

Page 26: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Coefficient of Restitution e

e = 1 : Perfectly elastic impact

e = 0 : Plastic impact / inelastic impact

Page 27: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Ex

The bag A, having a mass of 6 kg, is released from rest at the position = 0o. After falling to = 90o, it strikes an 18 kg box B. If the coefficientof restitution between the bag and box is e = 0.5, determine

(i) the velocities of the bag and box just after impact(ii) the loss of energy during collision

Page 28: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Conservation of Energy

6 kg

Datum at = 0o

(i) the velocities of the bag and box just after impact

Page 29: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Conservation of Momentum

(i)

6 kg

Page 30: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Coefficient of restitution

(ii)

Solving (i) and (ii), (vA)2 = - 0.554 m/s = 0.554 m/s (vB)2 = 1.66 m/s

Page 31: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Loss of Energy

(ii) the loss of energy during collision

Page 32: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Oblique Impact

The particles move away withvelocities having unknown directionsand unknown magnitudes.

(vA)2,

(vB)2

2 2

If v1 velocities are known;

Page 33: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Ex

The smooth disks A and B, having a mass of 1 kg and 2 kg, respectively,collide with the velocities shown in the figure. If e = 0.75, determine the x and y components of the final velocity of each disk just after collision.

Page 34: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

x components

y components

Page 35: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Conservation of “x” Momentum

(i) for x components of the final velocity;

(i)

Page 36: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Coefficient of Restitution (x)

Both disk are assumed to have components of velocity in the +x direction after collision

(ii)

Page 37: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

Solving (i) and (ii),

Ans.

Ans.

(i) for x components of the final velocity;

Page 38: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

(ii) for y components of the final velocity;

Conservation of “y” Momentum

Page 39: T 1 +  U 1-2 = T 2 Conservation of Energy Principle of Work and Energy

A man kicks the 200g ball such that it leaves the ground at an angle of 30oWith the horizontal and strikes the ground at the same elevation a distance of 15m away. Determine the impulse of hiss foot F on the ball. Neglect theImpulse caused by the ball’s weight while its being kicked.