1 / 7

Sect. 11.4: Conservation of Angular Momentum

Sect. 11.4: Conservation of Angular Momentum. Recall Ch. 9 : Starting with Newton’s 2 nd Law in Momentum form : ∑ F ext = (dp tot /dt)  For an isolated system with no external forces: ∑ F ext = 0 so (dp tot /dt) = 0  p tot = constant or

werner
Télécharger la présentation

Sect. 11.4: Conservation of Angular Momentum

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Sect. 11.4: Conservation of Angular Momentum

  2. Recall Ch. 9:Starting with Newton’s 2nd Law in Momentum form: ∑Fext = (dptot/dt) For an isolated system with no external forces: ∑Fext = 0 so (dptot/dt)= 0 ptot = constant or In the absence of external forces, the total momentum of the system is conserved. • Following the translational – rotational analogies we’ve been talking about all through Ch. 1: Consider the most general form of Newton’s 2nd Law for Rotations: • Consider the case with no external torques: ∑τext= 0 so (dLtot/dt)= 0 Ltot = constant or In the absence of external torques, the total angular momentum of the system is conserved.

  3. Conservation of Angular Momentum In the absence of external torques, the total angular momentum of the system is conserved. That is,Ltot = constant = Linitial = Lfinal(1) • If the mass of an isolated system is redistributed, the moment of inertia changes. In this case, conservation of angular momentum, Linitial = Lfinal requires a compensating change in the angular velocity. That is, (1) requires: Iiωi = Ifωf = constant • This holds for rotation about a fixed axis and for rotation about an axis through the center of mass of a moving system • Note that this requires that the net torque must be zero

  4. Example: Ice skater • Iiωi = Ifωf = constant But I =∑(mr2)  Iiωi = Ifωf (1) Between the left figure & the right one, he redistributed the distances of part of his mass from the axis of rotation.  I =∑(mr2) changes because the r’s change. (1) requires a compensating change inω. a b

  5. Example 11.8: Merry-Go-Round • Merry-Go-Round:Assume ideal disk. M = 100kg, R = 2 m, Im = (½)MR2 • Student:m = 60 kg.Is = mr2. As he walks to center, his r changes, soIschanges.Angular momentum is conserved, so angular speed ω must also change. • We have: Iiωi = Ifωf (1) Im + Is = (½)MR2 + mr2 • Initially, he is on the edge at r = R = 2 m. At that time, ωi = 2 rad/s. Finally, he is at r = 0.5 m. Find ωf. Use (1): [(½)MR2 + mR2]ωi = [(½)MR2 + mr2]ωf Put in numbers & solve: ωf = 4.1 rad/s

  6. Example: Diver Iiωi = Ifωf = constant Angular momentum is conserved throughout her dive.

  7. Conceptual Example Conservation of angular momentum!! Linitial = Lfinal L = - L + Lperson  Lperson = 2 L Demonstration!

More Related