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Physics 1901 (Advanced)

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Physics 1901 (Advanced) Prof Geraint F. Lewis Rm 560, A29 gfl_at_physics.usyd.edu.au www.physics.usyd.edu.au/~gfl/Lecture – PowerPoint PPT presentation

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Title: Physics 1901 (Advanced)


1
Physics 1901 (Advanced)
  • Prof Geraint F. Lewis
  • Rm 560, A29
  • gfl_at_physics.usyd.edu.au
  • www.physics.usyd.edu.au/gfl/Lecture

2
Gyroscope
3
Gyroscope Not rotating
4
Gyroscope Rotating
5
Precision Speed
  • Over a small time interval, there is a change in
    angular momentum given by

As dL is perpendicular to L, only the direction
of L changes, not magnitude.
6
Gravitation
7
Using Gravitation
  • Newton realised that using his gravitational
    formula was actually pretty tricky. If we have a
    randomly shaped object, what is the force it
    produces on a test (small) mass locate near by?

8
Using Gravitation
  • Newton realised that a spherical shell of matter
    has special properties. If you are outside the
    shell, he was able to show that the gravitational
    force was the same as if all the mass were
    concentrated at the centre of the shell (Rev.
    12.6)

Hence any spherical symmetric body (ie built of a
series of shells) behaves as if all the mass were
concentrated at the centre of the shells. Newton
realised he could treat planets as basically
being points! What about inside a spherical shell?
9
Weight
  • At the surface of the Earth

We know RE, g and G, so can calculate ME
10
Falling through the Earth
  • Assume a mass is dropped down a tunnel in a
    uniform density Earth. What is its equation of
    motion? How long does it take to return?

We have a wave equation again!
11
Gravitational Potential Energy
  • Imagine bringing two mass from far apart to close
    together. There is a change in the gravitational
    potential given by (remember work done and
    potential energy in a uniform gravitational
    field).

12
Escape Velocity
  • Imagine a projective is fired straight up. How
    fast must it be traveling not to fall back?
  • Using conservation of energy
  • Earth 11km/s
  • Sun 618km/s
  • Neutron star 200000km/s

13
Motion of Satellites
  • Gravity provides a centripetal acceleration. If a
    satellite has the correct velocity, v, it will
    move in a circular orbit, continually falling
    towards the Earth, but not getting any closer.

14
Motion of Satellites
  • The period of the orbit is

With this, you can calculate the period for a
geostationary orbit. The total energy is
is negative! Orbit is bound.
15
Non-circular Orbits
  • What if the velocity is too small for circular
    motion?
  • There is to much centripetal force and the
    objects radial position changes. By conservation
    of energy, it speeds up, then being too fast for
    circular motion.

Newton showed that the resultant motion is
elliptical, or if the velocity is much greater
than circular, the orbit is unbound and
hyperbolic. (The derivation is straight forward
and can be found at ??????????????????????????????
????)
16
Keplers 1st Law
  • Before Newton derived the mathematical form of
    orbits, Kepler determined three empirical laws .
  • His 1st Law says that orbits in the solar system
    are elliptical, with the Sun at one focus.

17
Is this always true?
  • A pair of equal mass stars will orbit their
    centre of mass (the barycentre), apparently
    orbiting nothing at all!
  • What motion do you expect the barycentre to have?

Borrowed from Wikipedia
18
Keplers 2nd Law
  • The 2nd Law says that the area an orbit sweeps
    out in a fixed time is a constant.

19
Keplers 2nd Law
  • Remember that the angular momentum is

For an elliptical orbit, r and ? are continually
changing, but L remains a constant. Given this,
we see that
Keplers 2nd Law is simply an expression of the
conservation of angular momentum.
20
Keplers 3rd Law
  • Keplers 3rd Law is relates the period of an
    elliptical orbit with semi-major axis a

Note that this is not dependent upon the mass of
the orbiting object.
http//hyperphysics.phy-astr.gsu.edu/hbase/kepler.
html
21
Orbits
The Solar System
The Galactic Centre
22
Orbits In general
  • In general, mass distributions are not point-like
    or spherical, so the overall potential does not
    have a 1/R form.
  • It turns out that closed elliptical orbits only
    occur in 1/R potentials, and generally orbits are
    more complicated, often having rosette-like
    patterns and are often not closed!

23
Round Up
  • This is the end of mechanics, and you should now
    be familiar with the concepts of force, momentum,
    energy and the action of gravity.
  • Remember, that it is important to understand the
    underlying concepts and build on these to
    understand the evolution of physical systems.
  • The laws of mechanics are universal and can be
    applied throughout science and the Universe.

24
  • THE END
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