Title: Modelling Pendulums
1Modelling Pendulums
- Pendulum - A body suspended from a fixed support
so that it swings freely back and forth under the
influence of gravity. Commonly used to regulate
various devices, especially clocks. - From the Latin pendulus meaning hanging.
2Aims
- Model a simple pendulum.
- Investigate whether the model is realistic, and
make necessary improvements. - Find a solution to the equation of motion.
- Look at modelling other systems related to the
simple pendulum. - Use techniques from senior school, A level, and
degree.
3PERIOD - time taken to complete one full
swing. What affects the period?
Equation of motion must include g and l, but not
m.
4Galileos findings
- Pendulums nearly return to their release heights.
- All pendulums eventually come to rest, with the
lighter ones coming to rest faster. - The period is independent of the bob weight.
- The period is independent of the amplitude.
- The square of the period varies directly with the
length.
5Assumptions
- Weight of string can be ignored
- String is inextensible
- Pendulum bob can be modelled as point mass
- No air resistance
- No friction
- Constant gravity, g9.80665
6Identify the forces and acceleration, parallel
and perpendicular to the string.
Apply Newtons second law, Fma, perpendicular to
string
d2? -g sin? dt2 l
7For small oscillations d2? ? -g ? dt2 l
Simple harmonic motion d2x -n2x dt2
Period of SHM 2?
n Period of pendulum 2? ?l
?g
8Other pendulum systems
Use Lagrangian mechanics -only need to find
kinetic and potential energies of the system to
find the equation of motion. NORMAL MODES-
particular solutions which oscillate with a
single frequency.
- Double pendulum
- Coupled oscillator
9Back to simple pendulum... Equation of
motion d2? -g sin? dt2 l Analyse as a
dynamical system and draw phase portrait.
Pendulum will never come to rest!
10Implies our assumptions are wrong. Introduce
damping factor d2? -g sin? - ?d? dt2 l
dt
Better model, but still not perfect.
11Finding a solution
Find ?(t) that satisfies our equation of
motion ? 2 sin-1 (sin½? sn(??t, sin½?)) where
sn is a Jacobi elliptic function. Also use
elliptic functions to find an expression for the
period (not just for small oscillations).
12Foucault Pendulum
1851 - Foucault uses a pendulum to show that the
earth rotates. 1954 - Maurice Allais reports that
a Foucault pendulum exhibits peculiar movement
during a solar eclipse.
13- Found equation of motion for the simple pendulum.
- Newtons second law.
- Dynamical Systems.
- Model wasnt realistic - add damping term.
- Solution to equation of motion, and expression
for the period. - Elliptic Functions.
- Looked at double pendulum and coupled oscillator.
- Lagrangian Mechanics.