Oscillations and Waves
What is a wave?
How do the particles move?
Some definitions…
1) Amplitude – this is “how high” the wave is:
2) Wavelength (λ) – this is the distance between two corresponding points on the wave and is measured in metres:
3) Frequency – this is how many waves pass by every second and is measured in Hertz (Hz)
Define the terms displacement, amplitude, frequency and period.
Describing waves
T
T
Time
Displacement
ω = 2π/T
f = 1/T
ω = 2πf
2π
1 cycle is described by 2π radians of phase
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What are radians?
Hyperlink and scroll down
Phase and angle
Examples of phase difference
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Oscillations
Simple harmonic motion
Any motion that repeats itself after a certain period is known as a periodic motion, and since such a motion can be represented in terms of sines and cosines it is called a harmonic motion.
The following are examples of simple harmonic motion:
a test-tube bobbing up and down in water (Figure 1)�a simple pendulum�a compound pendulum�a vibrating spring�atoms vibrating in a crystal lattice�a vibrating cantilever�a trolley fixed between two springs�a marble on a concave surface�a torsional pendulum�liquid oscillating in a U-tube�a small magnet suspended over a horseshoe magnet�an inertia balance
Data loggers
Analysing your graphs
SHM definition
SHM
Free body diagram for SHM
http://www.acoustics.salford.ac.uk/feschools/waves/shm2.htm
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Spring pendulum
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Oscillations to wave motion
Restoring forces
Simple Harmonic Motion
Consider a pendulum bob:
Let’s draw a graph of displacement against time:
Displacement
Time
Equilibrium position
“Sinusoidal”
Pendulum
Hyperlink
SHM Graphs
Time
Displacement
Velocity
Acceleration
Time
Time
T
Definition of SHM
Acceleration
Displacement
Now write your OWN definition of SHM
The Maths of SHM
Time
Displacement
Therefore we can describe the motion mathematically as:
x = x0cosωt
v = -x0ωsinωt
a = -x0ω2cosωt
a = -ω2x
Students are expected to understand the
significance of the negative sign in the equation
and to recall the connection between ω and T.
ω = 2π/T
SHM questions
a
x
5
2
a
x
Questions
When do you use cos or sin?
4.2 Energy changes during simple harmonic motion (SHM)
Energy
Displacement (x)
-x0
x0
At which points are
-max displacement?
-max velocity?
-max acceleration?
- max Ek
-max Ep
-max total energy?
Total energy
SHM: Energy change
Equilibrium position
Energy
Time
GPE
K.E.
Energy formulae
Energy
Displacement (x)
-x0
x0
Total energy
Ek = ½ mω2(x02 – x2)
Ep = ½ mω2x2
Etotal = ½ mω2x02
Questions
Answers
4.3 Forced oscillations and resonance
4.3.1 State what is meant by damping.
“It is sufficient for students to know that damping
involves a force that is always in the opposite
direction to the direction of motion of the
oscillating particle and that the force is a dissipative force.”
Free and Forced oscillations
Forcing frequency too slow
Forcing frequency too fast
Forcing frequency equals natural frequency
Resonance
Resonance and frequency
Hyperlink
Resonance and frequency
The width of the curve (Q value) is determined by the damping in the system. The value of the resonant frequency depends factors such as the size of the object…..
Tacoma Narrows
Useful resonance
Damping
Damped oscillations
Damping
Amplitude of driven system
Driver frequency
Low damping
High damping
Damping
How much damping is best?
Critical damping
Wave characteristics
The wave pulse transfers energy
If the source continues to oscillate, then a continuous progressive wave is produced.
Students should be able to distinguish between oscillations and wave motion, and appreciate that in many examples, the oscillations of the particles are simple harmonic.
Travelling Waves
Definition: A travelling wave (or “progressive wave”) is one which travels out from the source that made it and transfers energy from one point to another.
Energy dissipation
Clearly, a wave will get weaker the further it travels. Assuming the wave comes from a point source and travels out equally in all directions we can say:
Energy flux =
(in Wm-2)
Power (in W)
Area (in m2)
φ =
P
4πr2
An “inverse square law”
Example questions
State that progressive (travelling)�waves transfer energy.
Students should understand that there is no net motion of the medium through which the wave travels.
Transverse vs. longitudinal waves
Transverse waves are when the displacement is at right angles to the direction of the wave…
Longitudinal waves are when the displacement is parallel to the direction of the wave…
Displacement
Direction
Direction
Displacement
Transverse wave
Transverse waves
Students should describe the waves in terms of the direction of oscillation of particles in the wave relative to the direction of transfer of energy by the wave. Students should know that light waves and water waves are transverse and that water waves cannot be propagated in gases or liquids.
Longitudinal waves
Sound waves and earthquake P-waves are longitudinal
Longitudinal slinky
Loudspeaker
Describe waves in two dimensions,�including the concepts of wavefronts�and of rays.
Energy is transferred in 2 dimensions
Watch the wavefront(s) propagate
Wavefronts and rays
.
Wavefronts and rays
Rays show the direction of travel of the energy. The wavefronts are where the crests of the waves are. The rays are always at 90 deg to the wavefronts.
rays
Wavefronts
Longitudinal waves
Compressions and rarefactions
Transverse waves
Crests
Troughs
Displacement graphs
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Define the terms displacement, amplitude, frequency, period,�wavelength, wave speed and intensity
WAVELENGTH
- the distance from one crest to another or one trough to another. (In fact generally from any point on the wave to the next exactly similar point i.e. 2 consecutive points in phase)
FREQUENCY
- the number of vibrations of any part of the wave per second. The bigger the frequency the higher the pitch of the note or the bluer the light��AMPLITUDE
- the maximum distance that any point on the wave moves from its mean position. The bigger the amplitude the louder the sound, the rougher the sea, or the brighter the light
Period (T)
The time it takes for one complete cycle of the wave.
Displacement (x)
How far the “particle” has travelled from its mean position.
Wave speed (v)
The speed at which the wavefronts pass a stationary observer
Intensity (I)
The power per unit area that is received by an observer. Students should know that intensity α amplitude2
Derive and apply the relationship between wave speed, wavelength and frequency.
Speed = Dist/time
For 1 cycle of the wave, dist = λ and time =T
Speed = λ/T f = 1/T
Therefore V=fxλ
The Wave Equation
The wave equation relates the speed of the wave to its frequency and wavelength:
Wave speed (v) = frequency (f) x wavelength (λ)
in m/s in Hz in m
V
λ
f
Some example wave equation questions
0.2m
0.5m
0.6m/s
3x108m/s
Electromagnetic waves
Click to play
4.5 Wave properties
Wave diagrams
1) Reflection
4) Diffraction
3) Refraction
2) Refraction
The amount of transmission and reflection depends upon the difference in the “density” of the 2 media. i.e the bigger the difference, the greater the amount of reflection.
Refraction through a glass block:
Wave slows down and bends towards the normal due to entering a more dense medium
Wave speeds up and bends away from the normal due to entering a less dense medium
Wave slows down but is not bent, due to entering along the normal
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Finding the Critical Angle…
1) Ray gets refracted
4) Ray gets internally reflected
3) Ray still gets refracted (just!)
2) Ray still gets refracted
THE CRITICAL ANGLE
Optical fibres
Uses of Total Internal Reflection
Optical fibres:
An optical fibre is a long, thin, _______ rod made of glass or plastic. Light is _______ reflected from one end to the other, making it possible to send ____ chunks of information
Optical fibres can be used for _________ by sending electrical signals through the cable. The main advantage of this is a reduced ______ loss.
Words – communications, internally, large, transparent, signal
Other uses of total internal reflection
1) Endoscopes (a medical device used to see inside the body):
2) Binoculars and periscopes (using “reflecting prisms”)
Huygen’s principle
Snell’s law
Questions
Diffraction
More diffraction if the size of the gap is similar to the wavelength
More diffraction if wavelength is increased (or frequency decreased)
Diffraction
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Sound can also be diffracted…
The explosion can’t be seen over the hill, but it can be heard. We know sound travels as waves because sound can be refracted, reflected (echo) and diffracted.
Diffraction depends on frequency…
A high frequency (short wavelength) wave doesn’t get diffracted much – the house won’t be able to receive it…
Diffraction depends on frequency…
A low frequency (long wavelength) wave will get diffracted more, so the house can receive it…
i) Diffraction by a "large" object |
| ii) Diffraction at a "large" aperture |
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iii) Diffraction by a "small" object |
| iv) Diffraction by a "narrow" aperture |
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Superposition
Superposition is seen when two waves of the same type cross. It is defined as “the vector sum of the two displacements of each wave”:
Superposition
Interference of 2 pulses
Click to play
Constructive interference i.e. Loud or bright. Waves are in phase
Destructive interference i.e. dark or quiet. Waves are π rads out of phase.
Interference of sound waves
Where are the positions of constructive and destructive interference?
Interference of 2 point sources
Click to play
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Superposition patterns
Consider two point sources (e.g. two dippers or a barrier with two holes):
Superposition of Sound Waves
Path Difference
Constructive interference
Destructive interference
Max
1st Max
1st Max
Min
Min
2nd Max