Download presentation
Presentation is loading. Please wait.
Published byClaire Norman Modified over 9 years ago
2
Wave Physics PHYS 2023 Tim Freegarde
3
2 Wave propagation waves are collective bulk disturbances, in which motion is a delayed response to neighbouring motions the amplitudes are added when propagation follows multiple routes waves propagate via all possible routes
4
3 Huygens’ wave construction wavefronts propagate from initial disturbance in all directions Christiaan Huygens (1629-1695) each point on the wavefront acts as a secondary source further wavefronts propagate from the secondary sources in the same fashion where wavefronts coincide (strong constructive interference), a new wavefront is formed
5
4 4 Diffraction S Yoshioka & S Kinoshita, Forma 17 169 (2002) irridescence of feathers (Grimaldi, 1665)
6
5 5 Diffraction
7
6 6 Young’s double slit diffraction x ϑ amplitude intensity
8
7 7 Single slit diffraction x
9
8 8 x amplitude intensity ϑ
10
9 9 Diffraction grating x place secondary sources along wavefront...and trigger when wavefront arrives apply to sinusoidal waves by taking into account the phase with which components arrive combine by adding the amplitudes contributions may therefore interfere constructively or destructively INTERFERENCE
11
10 Diffraction gratings newport.com
12
11 Diffraction gratings newport.com m=0 m=1 m=2 m=-1 m=-2
13
12 Phased-array loudspeakers Croke Park, Dublin duran-audio.com AXYS
14
13 Phased-array radar Fylingdales, Yorkshire 2560 transducers, 25m diameter, 420-450 MHz
15
14 Towed array sonar typically 100 hydrophones over 300m 1500 m.s -1 seawater; 1435 m.s -1 freshwater www.surtass-lfa-eis.com
16
15 Spatial light modulators 1920 x 1200 pixels, LCD technology 8.1 μm pitch www.holoeye.com
17
16 Spatial light modulators 1920 x 1200 pixels, LCD technology 8.1 μm pitch www.holoeye.com laser tweezing of 2 μm glass spheres in fluid computer-controlled hologram www.physics.gla.ac.uk/optics projected and viewed through microscope
18
17 Michelson interferometer interference by division of amplitude beamsplitterdetector source δxδx
19
18 Michelson interferometer interference by division of amplitude beamsplitterdetector source δxδxδxδx sodium doublet optique-ingenieur.org chemistry.oregonstate.edu FTIR: Fourier transform infrared
20
19 Beating TWO DIFFERENT FREQUENCIES
21
20 Newton’s rings diffuser beam-splitter lens plate apply to sinusoidal waves by taking into account the phase with which components arrive combine by adding the amplitudes contributions may therefore interfere constructively or destructively www.sciencebuddies.org
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.