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Impulse and momentum student

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Impulse and Momentum Work & Energy • Scalar equation. The concept of work relates force to displacement. Greater force or greater displacement is associated with more work done. • More work done changes the motion of a system to a greater degree. • That which is changed is called kinetic energy. Work & Energy Impulse & Momentum • Vector equation. The concept of impulse relates force to time. Greater force or greater time of action is associated with more impulse applied. • More impulse changes the motion of a system to a greater degree. • That which is changed is called momentum. Impulse & Momentum Principle of Linear Impulse and Momentum Consider Newton’s 2nd law. Disediakan oleh SHAIFUL ZAMRI, JKM, POLIMAS
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Page 1: Impulse and momentum student

Impulse and Momentum

Work & Energy• Scalar equation.• The concept of work relates force to displacement.• Greater force or greater displacement is associated with more work done.• More work done changes the motion of a system to a greater degree.• That which is changed is called kinetic energy.Work & Energy

Impulse & Momentum• Vector equation.• The concept of impulse relates force to time.

• Greater force or greater time of action is associated with more impulse applied.• More impulse changes the motion of a system to a greater degree.• That which is changed is called momentum. Impulse & Momentum

Principle of Linear Impulse and Momentum

Consider Newton’s 2nd law.

Disediakan oleh SHAIFUL ZAMRI, JKM, POLIMAS

Page 2: Impulse and momentum student

Components of Impulse

Rectangular coordinate system

The final momentum of a particle is obtained by adding vectorially its initial momentum and the impulse of the force F acting during the interval considered.

Conservation of Linear Momentum

When the sum of the external impulses acting on a system of particle is zero, the equation for the principle of linear impulse and momentum reduces to the following:

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Page 3: Impulse and momentum student

Consider two boats initially at rest, which are pulled together

Impulsive forces and Motion

Impulsive force is a force that acts on a particle during a very short time interval and produces a definite change in momentum. The resulting motion is called an impulsive motion. Baseball hitting a bat.

Non impulsive forces like weight of the body, the force exerted by spring, or any other force which is known to be small compared with the impulsive force may be neglected.

In case of the impulsive motion of several particles, we can write:

No impulsive external forces acting on the body

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Page 4: Impulse and momentum student

Example

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Page 5: Impulse and momentum student

Example

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Page 6: Impulse and momentum student

Disediakan oleh SHAIFUL ZAMRI, JKM, POLIMAS

Page 7: Impulse and momentum student

Impact

Impact is a collision of two bodies, in a short interval of time, producing a large force between them.

Normal to the tangent line at the contact point is called the line of impact

Direct central impact

• The mass centers of the two bodies are on the line of impact• The impact velocities of the two bodies are directed along the line of impact

Oblique central impact

• The impact velocities of the two bodies are not directed along the line of impact

Direct Central Impact

Consider the impact of two particles

The total momentum of the two particles is conserved

Scalar components

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Page 8: Impulse and momentum student

Velocities after the Impact & the Coefficient of Restitution (e)

To obtain a second relationship between velocities, consider the motion of particle A and B during the period of deformation and apply the principle of impulse and momentum.

Particle A

Forces P and R are exerted on particle B and on particle A, in general R is different than P

The ratio of the magnitude of the impulses corresponding to the period of restitution and to the period of deformation is called the coefficient of restitution, e is always between 0 and 1.

Substitute for the impulses

Same approach for particle B gives:

Eliminate u

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Page 9: Impulse and momentum student

The following two equations can be used to determine the velocities of the particles after the impact.

Sign convention

The equations were derived assuming that particle B is located on the right of particle A and both particles are initially moving to the right. If particle B is moving to the left a negative sign should be considered. Same sign convention holds for after the impact.

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Page 10: Impulse and momentum student

example

A 20,000 kg railroad car moving at a speed of 0.5 m/s to the right collides with a 35,000 kg car which is at rest. If after the impact the 35,000 kg car is observed to move to the right at a speed of 0.3 m/s, determine the coefficient of restitution between the two cars.The total momentum of the two cars is conserved.

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Page 11: Impulse and momentum student

Example

A ball is thrown against a frictionless, vertical wall. Just before the ball strikes the wall, its velocity has a magnitude v and forms an angle of 30o with the horizontal. If the coefficient of restitution between the ball and wall is 0.9, determine the magnitude and direction of the velocity of the ball as it rebounds from the wall.

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