PHY 102 Waves Quanta Topic 4 Standing Waves

PHY 102: Waves & Quanta Topic 4 Standing Waves John Cockburn (j. cockburn@. . . Room E 15)

• Wave reflection at boundaries • Principle of superposition, interference • Standing waves on a string • Normal modes

Reflection of a wave pulse at a boundary time Pulse incident from right is reflected from the boundary at left HOW the pulse is reflected depends on the boundary conditions For fixed end, reflected pulse is inverted For free (in transverse direction) end, reflected pulse is same way up. Frictionless sliding ring Fixed end Free end

Reflection of a wave pulse at a boundary Behaviour at interface can be modelled as sum of two pulses moving in opposite directions at the interface: Transverse force always 0 at interface “fixed end” Transverse displacement always 0 at interface “free end”

Principle of superposition When 2 (or more) waves overlap in time/space, the total effect is just the algebraic sum of the individual wave functions: (must be so, because wave equation is linear: if y 1(x, t) and y 2(x, t) are both solutions, for example, then y 1+y 2 must also be a solution)

Formation of standing wave on a string Pink line represents wave travelling from right to left along the string. Blue line represents wave travelling from left to right. (wave reflection at boundaries) • Black line = sum of left and righttravelling waves = STANDING WAVE • Constructive interference of waves at ANTINODE of standing wave (max displacement) • Destructive interference of waves at NODE of standing wave (zero displacement) • Distance between successive nodes/antinodes = λ/2

Mathematical formulation of standing wave Wave moving right to left (pink wave) Wave moving left to right (blue wave) Total wave function (black wave):

Mathematical formulation of standing wave

Mathematical formulation of standing wave amplitude depends on position Zero y-displacement (node) when sin(kx) = 0 Maximum y-displacement (y=2 A) when sin(kx)=+/- 1……. .

Comparison between standing wave and travelling wave Travelling wave Standing wave particles undergo SHM all particles have same amplitude adjacent particles have different amplitude all particles have same frequency, all particles have same frequency adjacent particles have different phase all particles on same side of a node have same phase. Particles on opposite sides of node are in antiphase

Some very basic physics of stringed instruments……….

The fundamental frequency determines the pitch of the note. the higher harmonics determine the “colour” or “timbre” of the note. (ie why different instruments sound different)

Fundamental wavelength = 2 L From v = fλ, f 1= v/2 L So, for a string of fixed length, the pitch is determined by the wave velocity on the string…. .

Example Calculation The string length on standard violin is 325 mm. What tension is required to tune a steel “A” string (diameter =0. 5 mm) to correct pitch (f=440 Hz)? Density of steel = 8 g cm

Changing the “harmonic content” Plucking a string at a certain point produces a triangular waveform, that can be built up from the fundamental plus the higher harmonics in varying proportions. Plucking the string in a different place (or even in a different way) gives a different waveform and therefore different contributions from higher harmonics (see Fourier analysis) string plucked here This makes the sound different, even though pitch is the same…………………