1. Sect. 11.4: Conservation of Angular Momentum

2. the total angular momentum of the system is conserved.
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)
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 in ω. 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,
so Is changes. 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!