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ENSC2004 - Lecture 20
Impulse and Momentum (Rigid Bodies) - Slides

Linear and Angular Momentum

  • The linear momentum of a rigid body is mass times speed:

    This equation states that the linear momentum vector has a magnitude equal to () and a direction defined by
  • The angular momentum of a rigid body is inertia times angular velocity:

    When body undergoes purely rectilinear or curvilinear translation, thus, angular momentum is zero ()

When a rigid body is rotating about a fixed axis passing through , then:

The equations above still apply

When a rigid body is subjected to general plane motion, both the linear momentum and the angular momentum computed about G are required


The angular momentum about point A is:

Principle of Impulse and Momentum

  • Force → creates impulse → creates change in momentum
  • Use these equations to solve problems with force, velocity, and time

Linear impulse-linear momentum equation:

Angular impulse-angular momentum equation:


Conservation of Momentum 2 - Slides

Conservation of Momentum 2

  • Recap: Conservation of Linear & Angular Momentum
  • ! When linear impulses are negligible or non-impulse, we can use the conservation of linear momentum to solve problems
    • You can identify negligible forces if they act over a very short/instantaneous period of time
  • See example in slides

End of Unit!