Tuesday, 19 September 2023

Week 10 Term 3 2023 Part 3

 Homework

  • Act 4A, p.56 Properties of Waves
  • Act 5A, p.73-74 Standing Waves
  • Act 5B, p.79-80 Music

  • Ex 3D, p.75-79, Standing Waves and Music

  • Act 6A, p.85-86 The Doppler Effect
  • Ex 3E, p.81-84, Beats

  • Ex 3A, p. 50-53 Basic Wave Properties

  • Ex 3B, p. 57-63 Two Point Source Interference

  • Ex 3C, p. 66-70 Multi Point Source Interference


Two Point Source Interference


nšœ† = dsin(š›³)

Double Slit App - Physics Classroom



Wave-Particle Duality Applied to the Double Slit Experiment

Diffraction Grating of White Light 
(Multi-Point Source Interference)

Green vs White Light Diffraction


Multiple Point Source Interference





Thin Film Interference


Thin Film Interference



Making Colour with Holes


Why Blue is so rare



Visible Spectrum

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Week 10 Term 3 2023 Part 2

  Homework

  • Act 4A, p.56 Properties of Waves
  • Act 5A, p.73-74 Standing Waves
  • Act 5B, p.79-80 Music

  • Ex 3D, p.75-79, Standing Waves and Music

  • Act 6A, p.85-86 The Doppler Effect
  • Ex 3E, p.81-84, Beats

Doppler Effect





The Doppler Effect: what does motion do to waves?

Doppler Effect

Intro to the Doppler Effect

Doppler Effect Observed Frequency Equation

Sonic Boom

Doppler Shifting Song


Beats

two waves of a similar frequency (similar wavelength) superimpose to come in and out of phase causing constructive and deconstructive interference respectively. This causes a warbling/beat sound of frequency (fb) equal to the difference in respective frequencies

fb = | f1 - f2 |

Wave Beats

Easy Beats- Physics


Wine Glass Resonance in Slow Motion

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Week 10 Term 3 2023

 Homework

  • Act 4A, p.56 Properties of Waves
  • Act 5A, p.73-74 Standing Waves
  • Act 5B, p.79-80 Music

  • Ex 3D, p.75-79, Standing Waves and Music

  • Act 6A, p.85-86 The Doppler Effect


    • Longitudinal Waves

    Particle displacement in the medium is parallel to the direction of wave propagation e.g. sound waves, primary earthquake waves

    Transverse Waves
    Particle displacement in the medium is perpendicular to the direction of wave propagation e.g. light and other electromagnetic waves, secondary earthquake waves

    Frequency - Period


    Sound Waves
    Superposition of Waves

    Waves travel through each other and the total amplitude at any moment is equal to the sum of amplitudes of the individual waves.


    Standing Waves
    In musical instruments - when a reflected wave travels back through itself causing fixed points of Nodes (Deconstructive Interference) and Antinodes (Constructive Interference) due to the fractional relationship between the wavelength (šœ†) of the wave and the length (L) of the resonating chamber

    in musical instruments - when a reflected wave travels back through itself causing fixed points of Nodes (Deconstructive Interference) and Antinodes (Constructive Interference) due to the fractional relationship between the wavelength (šœ†) of the wave and the length (L) of the resonating chamber


    Harmonic
    String
    Double Open Ended Pipe
    Closed Ended Pipe
    1st
    šœ† = 2L
    f = f1st
    šœ† = 2L
    f = f1st
    šœ† = 4L
    f = f1st
    2nd
    šœ† = L
    f = 2f1st
    šœ† = L
    f = 2f1st

    3rd
    šœ† = ⅔ L
    f = 3f1st
    šœ† = ⅔ L
    f = 3f1st
    šœ† = 4/3 L
    f = 3f1st
    4th
    šœ† = ½ L
    f = 4f1st
    šœ† = ½ L
    f = 4f1st

    5th
    šœ† = ⅖ L
    f = 5f1st
    šœ† = ⅖ L
    f = 5f1st
    šœ† = ⅘ L
    f = 5f1st

    Standing Waves Part I: Demonstration


    Standing Waves Part II: Explanation

    Standing Waves


    Standing Waves on a String
    1st Harmonic
    2nd Harmonic
    3rd Harmonic
    4th Harmonic
    šœ† = 2L
    šœ† = L
    šœ† = ⅔ L
    šœ† = ½ L
    f = f1st
    f = 2f1st
    f = 3f1st
    f = 4f1st


    Standing Waves in a Pipe


    Standing Waves in a Wave Tank


    Standing Waves on a 2D Plate

    Cymatics

       Acoustic Levitation in ULTRA SLOW MOTION


    Timbre
    Timbre is caused by the shape of the repeating wave unit. This gives instruments their characteristic sound even when playing the same note

     Musical Notes and Frequencies
("Middle C" is C4 )

NoteFrequency (Hz)Wavelength (cm)
C016.352109.89
 C#0/Db0 17.321991.47
D018.351879.69
 D#0/Eb0 19.451774.20
E020.601674.62
F021.831580.63
 F#0/Gb0 23.121491.91
G024.501408.18
 G#0/Ab0 25.961329.14
A027.501254.55
 A#0/Bb0 29.141184.13
B030.871117.67
C132.701054.94
 C#1/Db1 34.65995.73
D136.71939.85
 D#1/Eb1 38.89887.10
E141.20837.31
F143.65790.31
 F#1/Gb1 46.25745.96
G149.00704.09
 G#1/Ab1 51.91664.57
A155.00627.27
 A#1/Bb1 58.27592.07
B161.74558.84
C265.41527.47
 C#2/Db2 69.30497.87
D273.42469.92
 D#2/Eb2 77.78443.55
E282.41418.65
F287.31395.16
 F#2/Gb2 92.50372.98
G298.00352.04
 G#2/Ab2 103.83332.29
A2110.00313.64
 A#2/Bb2 116.54296.03
B2123.47279.42
C3130.81263.74
 C#3/Db3 138.59248.93
D3146.83234.96
 D#3/Eb3 155.56221.77
E3164.81209.33
F3174.61197.58
 F#3/Gb3 185.00186.49
G3196.00176.02
 G#3/Ab3 207.65166.14
A3220.00156.82
 A#3/Bb3 233.08148.02
B3246.94139.71
C4261.63131.87
 C#4/Db4 277.18124.47
D4293.66117.48
 D#4/Eb4 311.13110.89
E4329.63104.66
F4349.2398.79
 F#4/Gb4 369.9993.24
G4392.0088.01
 G#4/Ab4 415.3083.07
A4440.0078.41
 A#4/Bb4 466.1674.01
B4493.8869.85
C5523.2565.93
 C#5/Db5 554.3762.23
D5587.3358.74
 D#5/Eb5 622.2555.44
E5659.2552.33
F5698.4649.39
 F#5/Gb5 739.9946.62
G5783.9944.01
 G#5/Ab5 830.6141.54
A5880.0039.20
 A#5/Bb5 932.3337.00
B5987.7734.93
C61046.5032.97
 C#6/Db6 1108.7331.12
D61174.6629.37
 D#6/Eb6 1244.5127.72
E61318.5126.17
F61396.9124.70
 F#6/Gb6 1479.9823.31
G61567.9822.00
 G#6/Ab6 1661.2220.77
A61760.0019.60
 A#6/Bb6 1864.6618.50
B61975.5317.46
C72093.0016.48
 C#7/Db7 2217.4615.56
D72349.3214.69
 D#7/Eb7 2489.0213.86
E72637.0213.08
F72793.8312.35
 F#7/Gb7 2959.9611.66
G73135.9611.00
 G#7/Ab7 3322.4410.38
A73520.009.80
 A#7/Bb7 3729.319.25
B73951.078.73
C84186.018.24
 C#8/Db8 4434.927.78
D84698.637.34
 D#8/Eb8 4978.036.93
E85274.046.54
F85587.656.17
 F#8/Gb8 5919.915.83
G86271.935.50
 G#8/Ab8 6644.885.19
A87040.004.90
 A#8/Bb8 7458.624.63
B87902.134.37
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