17 : Oscillations Flashcards
1
Q
oscillating motion
A
- object starts in equilibrium position a force is applied displacing it and causes it to oscillate
- it travels towards equilibrium position at and increasing speed it slows down when it goes past equilibrium position eventually reaching max displacement (amplitude) = 0 acceleration and speed
- max acceleration at equilibrium
2
Q
displacement
A
the distance from the equilibrium position
3
Q
amplitude
A
the maximum displacement from the equilibrium position
4
Q
period
A
the time taken to complete one full oscillation
5
Q
frequency
A
the number of complete oscillations per unit time
6
Q
angular frequency
A
- ω = 2π/T
- or ω = 2πf
7
Q
simple harmonic motion
A
- oscillates either side of a midpoint
- there is always a restoring force pulling or pushing back towards. the midpoint
- size of restoring force depends on displacement and force accelerates towards the midpoint
8
Q
conditions for SMH
A
- a = ω ^2 x
- acceleration of the object is directly proportional to its displacement
- acceleration of object acts opposite direction to the displacement
9
Q
restoring force
A
- type of potential force provides restoring ( gpe for pendulums or elastic pe for spring )
- as objects moves towards the midpoint restoring force does work on object transerferring pe to ke and when moving away from midpoint ke transfers to pe
- through midpoint pe is zero and ke is max
- at max displacement ke is zero and pe is max
- sum of pe and ke = mechanical energy and stays constant
10
Q
free vibrations
A
- stretch and release mass on spring it oscillates at is natural frequency
- if no energy transfers to surroundings it will keep oscillating with the same amplitude forever
11
Q
forced vibrations
A
- forced to oscillate by a periodic external force
- the frequency of this force is called driving frequency
12
Q
resonance
A
- when driving frequency approaches natural frequency the system gains more energy from the driving force and vibrates with rapidly increasing amplitude
- driving frequency = natural frequency
13
Q
Damping
A
- any oscillating system loses energy to its surroundings
- caused usual ly by frictional forces like air resistance
- systems are deliberately damped to stop them oscillating or to minimise effect of resonance
14
Q
degree of damping
A
- damping reduces the amplitude of the oscillation over time
- critical damping reduces amplitude in the shortest possible time
- even hever daping are overdamped and take longer to return to equilibrium
- plastic deformation of ductile materials reduces the amplitude of oscillations in the same way of damping as material changes shape it absorbs energy and oscillation will become smaller
15
Q
damping affecting resonance
A
- lightly damped systems have very sharp resonance peak amplitude only increases dramatically when he driving frequency is very close to natural frequency
- heavily damped systems have a flatter response amplitude doesn’t increase much er natural frequency and aren’t as sensitive to driving frequency