Title: Conservation of Angular Momentum
1(No Transcript)
2Conservation of Angular Momentum
Since
Consider
Note
Thus
Conclusion
The angular momentum of particle subject to no
torque is conserved.
3Work
- Definition (Just a reminder)
2
1
4Kinetic Energy
- To motivate the concept, consider
The work, W, can thus be expressed as an exact
differential.
Definition of Kinetic Energy
5Conservative Forces
If the work performed by a force while moving a
particle between two given (arbitrary) positions
is independent of the path followed, then the
work can be expressed as a function of the two
end points of the path.
Conservative Force or system
- Where we defined the functions Ui as the
potential energy of the particle at the location
i. - Note the signs
6Conservative Forces (contd)
- A force is conservative if it can be expressed a
the gradient of a scalar function U.
Verify by substitution
In most systems of interest,U is a function of
the position only, or position and time. We will
study central potentials in particular, and we
will not consider potentials that depend on
velocity.
7Conservative Forces (contd)
- Important notes about potentials.
- Potentials are defined only up to a constant
since
Potentials are known relative to a chosen
(arbitrary) reference. Choose reference position
and values to ease the solution of specific
problems. E.g. for 1/r potentials, choose U0 at
infinity.
8Conservative Forces (contd)
- Potential energy is thus NOT an absolute
quantity it does not have an absolute value. - Likewise, the Kinetic Energy is also NOT an
absolute quantity it depends on the specific
rest frame used to measure the velocity.
9Total Mechanical Energy
- Definition E T U.
- It is a conserved quantity!
- To verify, consider the time derivative
Recall
Thus
The time derivative of the potential can be
expressed as a sum of partial derivatives.
10Total Mechanical Energy (contd)
0
Conclusion if U is not an explicit function of
time, then the energy is conserved!
11Total Mechanical Energy (contd)
- In a conservative system, the force can be
expressed as a function of a gradient of a
potential independent of time. - The total mechanical energy, E, is thus a
conserved quantity in a conservative system. - The conservations theorem we just saw can be
considered as laws, but keep in mind they
strictly equivalent to Newtons Eqs 2 3. - Conservations theorems are elegant, and
powerful. - They led W. Pauli (1880-1958) to postulate (in
1930) the existence of the neutrino, as a product
of b-decay to explain the observed missing
momentum!
12Example Mouse on a fan
- Question A mouse of mass m jumps on the
outside of a freely spinning ceiling fan of
moment of inertia I and radius R. By what ratio
does the angular velocity change? - Answer
- Angular momentum must be conserved.
- Calculate the angular momentum before and after
the jump. - Equate them.
13Energy
- Concept of energy now more popular than in
Newtons time - Became clear early 19th century that other forms
of energy exist e.g. heat. - Rutherford discovered clear link between heat
generation and friction. - Law of conservation of energy first formulated by
Hermann von Helmholtz (1821-1894) based on
experimental work done largely by James Prescott
Joule (1818-1889).
14Use of Energy for problem solving.
1-D Case
This is a generic solution need U(x) and
integrate to get a function of t(x)...
15Energy (contd)
- Can learn a great deal without performing the
integration (which can get difficult). - Consider a plot of the energy and potential vs x.
EE4 - unbound motion
EE3 - 1 side bound, non periodic
EE2 - bound periodic motion
EE1 - bound periodic motion
16Energy (contd)
- Note Whenever motion is restricted near a
minimum of a potential, it may be sufficient to
approximate U(x) with a harmonic potential
approximation
U(x)
E
17Stable/Unstable equilibrium
- One can determine whether an equilibrium is
stable or unstable base on the curvature of the
potential at the equilibrium point.
Consider a Taylor expension of the potential
18Stable/Unstable equilibrium (contd)
- We have an equilibrium if
Near xo
Stable equilibrium if
Unstable equilibrium if
Higher orders to be considered if