Momentum and Conservation of Momentum Momentum Conservation of - - PDF document

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Momentum and Conservation of Momentum Momentum Conservation of - - PDF document

Momentum and Conservation of Momentum Momentum Conservation of Momentum Impulse-Momentum Theorem Homework 1 Momentum The linear momentum, p , of a particle with mass, m , moving with a velocity, v , is defined as p = m v


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Momentum and Conservation of Momentum

  • Momentum
  • Conservation of Momentum
  • Impulse-Momentum Theorem
  • Homework

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Momentum

  • The linear momentum, p, of a particle with mass, m,

moving with a velocity, v, is defined as p = mv

  • In general, the momentum, p, has three components

px = mvx py = mvy pz = mvz

  • Alternative statement of Newton’s 2nd law: The time

rate of change of momentum of a particle is equal to the net force acting on the particle. ΣF = dp dt

  • If the mass of the particle is constant, we get our pre-

vious expression for Newton’s 2nd law ΣF = dp dt = d (mv) dt = mdv dt = ma

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Conservation of Momentum

  • The total momentum for a system of particles is

ptot = Σpi = Σmivi

  • Applying Newton’s 2nd law, we have

ΣFext = dptot dt

  • If ΣFext = 0, then dptot

dt = 0 so that

ptot = constant

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SLIDE 4

Example 1

A bullet with a mass of 3.8 g is fired horizontally with a speed of 1100 m/s into a large block of wood with a mass of 12 kg resting on a frictionless surface. What is the speed of the block after impact?

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Example 1 Solution

A bullet with a mass of 3.8 g is fired horizontally with a speed of 1100 m/s into a large block of wood with a mass of 12 kg resting on a frictionless surface. What is the speed of the block after impact?

vf vi M M+m m Initial Final

pi = pf mvii = (M + m) vfi vf = m M + mvi vf = 3.8 × 10−3kg 12 kg + 3.8 × 10−3kg (1100 m/s) = 0.35 m/s

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Impulse-Momentum Theorem

  • Assume that a net force ΣF acts on a particle and that

it may vary with time as shown below

  • We can use Newton’s 2nd law to write the differential

change in momentum, dp, in the differential element

  • f time, dt, as

dp = ΣFdt

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Impulse-Momentum Theorem (cont’d)

We can integrate this expression to find the change in momentum, ∆p, of the particle during the time interval ∆t = tf − ti

pf

pi dp =

tf

ti ΣFdt

∆p = pf − pi =

tf

ti ΣFdt

The integral of force over the time interval during which it acts is a vector quantity called the impulse, I, defined by I ≡

tf

ti ΣFdt = ∆p

We can also express the impulse in terms of a time-averaged net force ΣF I = ∆p = ΣF∆t

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Example 2

A 0.14-kg baseball, in horizontal flight with a speed vi of 39 m/s, is struck by a batter. After leaving the bat, the ball travels in the opposite direction with a speed vf, also 39 m/s. (a) What impulse acted on the ball while it was in contact with the bat? (b) What average force acts on the baseball if the impact time is 1.2 ms?

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Example 2 Solution

A 0.14-kg baseball, in horizontal flight with a speed vi of 39 m/s, is struck by a batter. After leaving the bat, the ball travels in the opposite direction with a speed vf, also 39 m/s. (a) What impulse acted on the ball while it was in contact with the bat? (b) What average force acts on the baseball if the impact time is 1.2 ms? (a) I = pf − pi = mvfi − (−mvfi) = m(vf + vi)i I = (0.14 kg)(39 m/s + 39 m/s)i = 11 kg · m/s i (b) F = I ∆t = 11 kg · m/s i 0.0012 s = 9200 N i

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Homework Set 14 - Due Wed. Oct. 13

  • Read Sections 8.1-8.2
  • Answer Questions 8.3 & 8.9
  • Do Problems 8.1, 8.4, 8.7 & 8.10

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