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Published byBruno Scott Modified over 9 years ago
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Depends on relative motion of source and detector Closer = decr wavelength › Incr pitch › Blue shift Farther = incr wavelength › Decr pitch › Red shift
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EM waves do not require a medium Speed of light can be different for different observers One Doppler effect-it depends on the relative speed between the observer and the source Doppler radar-EM waves are sent out › Change in frequency of the reflected beam relative to the outgoing beam measures speed of clouds and precipitation that reflected the beam
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IB text (green) › P.299-300 ex 11.2(a) & (b) Walker Text (blue) › P.471 # 34, 35, 38, 42, 44, 45, 46, 84
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Fixed End › Inverted › 180 o change in phase Free End › Erect › In Phase
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Waves at a discontinuity, or boundary between different media › Part of wave is reflected. › Part of wave is transmitted into the new medium. › The “heavier”, or “more rigid”, or “denser” the second section: the more is reflected & less transmitted
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Principle of Superposition › The net effect of two causes is found by adding the individual effects of each cause. › Crest + Crest = one larger crest Constructive Interference › Crest + Trough = zero displacement Destructive Interference › Interference need not be complete
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Coherent Sources › Same frequency › In phase Nodes – complete destructive interference Antinodes – max constructive interference
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IB text (green) › P.124 ex 4.5(b) & P.442 ex 18.3 Walker Text (blue) › PP.471-472 #47-49, 51, 53, 55
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Two waves moving through a medium simultaneously will interfere › Speed depends on medium › If frequency is correct, interference will result in a waveform which appears to stand still
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Nodes – points of zero displacement Antinodes – points of maximum displacement Node Antinode
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Usually produced by reflected wave interfering with incident wave From rigid surface › Nodal points @ source & point of reflection Standing wave does not propagate energy
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IB text (green) › P.294 ex 11.1(a)
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Resonance › An oscillatory system is driven by a driving force that has a frequency equal to the natural frequency of oscillation of the system › Can be useful or harmful
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Resonant standing waves: harmonics › 1 st harmonic: fundamental
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Strings › Fixed end reflection = phase change 1 st harmonic: L = ½ λ 2 nd harmonic: L = λ 3 rd harmonic: L = ¾ λ 4 th harmonic: L = 2λ
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Laws of Strings › Law of Lengthsf = l ’ f’ l › Law of Diametersf = d ’ f’ d › Law of Tensionsf = √F f’ √F ’ › Law of densitiesf = √D ’ f’ √D
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Columns of air (pipes) › Closed end reflection phase change Node at the end Only odd harmonics are present 1 st harmonic: L = ¼ λ 3 rd harmonic: L = ¾ λ 5 th harmonic: L = 5 / 4 λ
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Columns of air (pipes) › Open end reflection No phase change Antinode at the end All harmonics are present 1 st harmonic: L = ½ λ 2 nd harmonic: L = λ 3 rd harmonic: L = 3 / 2 λ
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IB text (green) › P.297 ex 11.1(b) Walker Text (blue) › P.472 #57-59, 60, 63-65, 68
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