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standing/stationary waves
formed by the superposition of two waves that are:
same frequency, amplitude, speed, type (FAST)
opposite direction
results from progressive wave being reflected antiphase at a boundary → superposition of incident and reflected wave
nodes: points that always show no displacement (due to destructive interference)
antinodes: points that reach maximum amplitude of displacement (due to constructive interference)
distance between consecutive nodes (or antinodes) = λ/2
all particles between two nodes are in phase
standing vs travelling waves
phase
standing wave: all points between two nodes are in phase
travelling wave: all particles along a wavelength have different phase
amplitude
standing wave: all points on the wave have fixed amplitudes. max amplitude is fixed between zero (at nodes) and double the amplitude of component waves (at antinodes)
travelling wave: all points on the wave have the same amplitude
wavelength
standing wave: 2 x distance between adjacent nodes (or antinodes)
travelling wave: shortest distance between two points in phase
energy
standing wave: does not transmit energy, but there is an energy associated with it
travelling wave: transmits energy
wave pattern
standing wave: wave does not move
travelling wave: wave moves
boundary conditions
The number of nodes and antinodes that fit within the available length of medium depends on:
The frequency of the travelling waves
The boundary conditions (i.e. whether the travelling waves travel between two fixed ends, two free ends or a fixed and a free end) -. standing waves that meet these conditions is a possible resonant mode
for stretched strings
two fixed ends→ so the standing wave created must have a node at the fixed end.
travelling waves meeting a fixed boundary will be reflected anti-phase → forms standing wave
why open end of tube has standing wave?
pressure difference due to compressions/rarefactions → partially reflected in phase at free end since denser to less dense → forms standing wave
resonant frequencies
aka harmonics. frequencies of standing waves.
fn = n f1
fundamental frequency aka first harmonic: standing wave with lowest possible frequency
timbre/quality: depends on relative amplitude of different harmonics produced by the instrument
first harmonic of a 1.0m long stretched string is 650Hz, what will its first harmonic be if its length is shortened to 80cm, keeping tension constant?
first harmonic = 1.0m for stretched string (two nodes) → ½ λ
λ = 1.0 × 2 = 2.0m
v = fλ = 650 × 2 = 1300 → tension constant means v constant
λnew = 0.8 × 2 = 1.6
f1 = v/λ = 1300/1.6 = 812.5 Hz
resonance
resulting amplitude of system becomes maximum when driving frequency of external driving force = natural frequency of system. there is a maximum transfer of energy from the driving force to driven system.
natural frequency f0 depends on dimensions and nature of material
useful applications
musical instruments
radio receivers: tuner adjusted so that frequency of electrical oscillations in circuit is same as that of radio waves → amplifies signals of that radio wave + diminish radio waves of other frequencies
microwave oven: microwaves with frequency similar to natural frequency of vibration of water molecules → resonate, absorb energy from microwaves, heat up water in food (containers don’t heat up because they don’t have water molecules)
magnetic resonance imaging: strong varying radio frequency EM fields are used to cause oscillations in atomic nuclei → resonance, molecules absorb energy → analyse pattern of energy absorption, computer generates image
not useful applications
shattering of glass
earthquakes: buildings forced to oscillate in resonance with seismic waves, increased energy transfer causes more damage (solution: dampeners)
human internal organs resonate in response to external frequencies (usually < 10Hz) → high levels of vibration can damage heart/lungs/intestines/brain
damping
process where energy is taken from an oscillating system due to dissipative forces
frequency response graph
amplitude of oscillation against driving frequency
as driving frequency increases,
f < f0: amplitude of driven oscillating system increasing
f = f0: resonance, max amplitude
f increased further, f > f0, amplitude decreases
at resonance, theoretically infinite amplitude if there was no damping, because continuous input of energy
damping: amplitude/energy increases until rate of energy transfer = rate of dissipation
effect of damping on frequency response graph
amplitude of peak oscillation decreases
peak becomes broader, spreads over wider range of frequencies
resonance occurs at frequency smaller than f0
types of damping
light damping
oscillations are maintained about equilibrium position after system has been displaced. amplitude of oscillations decreases over a long time.
occurs for most oscillations
critical damping
no oscillations occur, motion is brought to rest in the shortest possible time
eg car suspension system
heavy/over-damping
no oscillations occur but system takes long time to return to equilibrium position compared to critically damped system, because damping force > critical amount
eg anti-slam doors
phase difference depending on f vs f0 (out of syllabus?)
f << f0 → in phase
resonance, f = f0 → phase difference π/2
f >> f0 —> anti-phase, phase difference π