A siren gets higher as it approaches, lower as it recedes
Source moving toward you β crests bunch up β higher frequency β higher pitch. Moving away β crests spread out β lower pitch. Used in radar, ultrasound, and astronomy.
Source moving toward you β crests bunch up β higher frequency β higher pitch. Moving away β crests spread out β lower pitch. Used in radar, ultrasound, and astronomy.
Transverse waves (light, water surface): particles move perpendicular to wave travel. Longitudinal waves (sound): particles compress and rarefy parallel to travel direction. Sound cannot travel through a vacuum β light can.
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Resonance
Resonance: driving frequency matches natural frequency β amplitude builds
Resonance
Push at the right frequency and things vibrate dramatically
Every object has a natural resonant frequency. Drive it at that frequency β amplitude grows. Tacoma Narrows Bridge (1940) is the classic example, though engineers now attribute its collapse to aeroelastic flutter rather than simple resonance. Basis of MRI, musical instruments, and radio tuning.
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π Resonance
What is resonance?
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π Answer
Resonance: driving frequency matches natural frequency β amplitude builds
Every object has a natural resonant frequency. Drive it at that frequency β amplitude grows. Tacoma Narrows Bridge (1940) is the classic example, though engineers now attribute its collapse to aeroelastic flutter rather than simple resonance. Basis of MRI, musical instruments, and radio tuning.
Standing waves form when reflected waves interfere constructively
A standing wave appears stationary but is really two waves traveling in opposite directions. Nodes: points of zero amplitude. Antinodes: points of maximum amplitude. String instruments and organ pipes use this principle.
A standing wave appears stationary but is really two waves traveling in opposite directions. Nodes: points of zero amplitude. Antinodes: points of maximum amplitude. String instruments and organ pipes use this principle.
Constructive interference: waves in phase, amplitudes add. Destructive interference: waves out of phase (180Β°), amplitudes subtract. Superposition principle: resultant wave = sum of individual waves. Beats: two slightly different frequencies β periodic loud/soft pattern = beat frequency = |fβ - fβ|.
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Sound Intensity and Decibels
Sound intensity: decibels (dB). Every 10 dB increase = 10Γ more intense. 20 dB = 100Γ more intense.
Sound Intensity and Decibels
The logarithmic scale of sound intensity
0 dB: threshold of hearing. 60 dB: normal conversation. 120 dB: threshold of pain. Every 10 dB increase represents a 10-fold increase in intensity. 20 dB increase = 10 Γ 10 = 100Γ more intense. Perceived loudness doubles roughly every 10 dB.
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π Sound Intensity and Decibels
Decibels β how does intensity scale?
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π Answer
Sound intensity: decibels (dB). Every 10 dB increase = 10Γ more intense. 20 dB = 100Γ more intense.
0 dB: threshold of hearing. 60 dB: normal conversation. 120 dB: threshold of pain. Every 10 dB increase represents a 10-fold increase in intensity. 20 dB increase = 10 Γ 10 = 100Γ more intense. Perceived loudness doubles roughly every 10 dB.
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Wave Properties Summary
Frequency determines pitch. Amplitude determines loudness. Speed depends on medium.
Wave Properties Summary
The relationship between frequency, amplitude, and speed
Frequency (Hz): number of complete cycles per second β determines pitch for sound, color for light. Amplitude: maximum displacement from equilibrium β determines loudness for sound, brightness for light. Speed: set by the medium β sound travels faster in solids than liquids than gases.
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π Wave Properties Summary
What do frequency, amplitude and speed determine?
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π Answer
Frequency determines pitch. Amplitude determines loudness. Speed depends on medium.
Frequency (Hz): number of complete cycles per second β determines pitch for sound, color for light. Amplitude: maximum displacement from equilibrium β determines loudness for sound, brightness for light. Speed: set by the medium β sound travels faster in solids than liquids than gases.
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Electromagnetic Waves
Electromagnetic spectrum: all EM waves travel at c = 3Γ10βΈ m/s in vacuum. In a medium, speed and wavelength change; frequency does not.
Electromagnetic Waves
What all EM waves have in common β and what distinguishes them
All EM waves: travel at c in vacuum, are transverse, require no medium. Radio waves: lowest frequency, longest wavelength. Gamma rays: highest frequency, most energy. In a medium (glass, water): speed slows, wavelength shortens, but frequency stays the same β this is why light bends at interfaces.
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π Electromagnetic Waves
EM waves β how fast, and what changes in a medium?
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π Answer
Electromagnetic spectrum: all EM waves travel at c = 3Γ10βΈ m/s in vacuum. In a medium, speed and wavelength change; frequency does not.
All EM waves: travel at c in vacuum, are transverse, require no medium. Radio waves: lowest frequency, longest wavelength. Gamma rays: highest frequency, most energy. In a medium (glass, water): speed slows, wavelength shortens, but frequency stays the same β this is why light bends at interfaces.
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Diffraction
Diffraction: waves bend around obstacles or through openings. More diffraction when wavelength β opening size.
Diffraction
Why waves spread out when they pass through gaps
Diffraction is most pronounced when the wavelength is comparable to the opening or obstacle size. Sound diffracts easily around corners (long wavelengths). Light diffracts less visibly (very short wavelength). Single slit and double slit diffraction patterns are classic exam problems.
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π Diffraction
Diffraction β when is it strongest?
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π Answer
Diffraction: waves bend around obstacles or through openings. More diffraction when wavelength β opening size.
Diffraction is most pronounced when the wavelength is comparable to the opening or obstacle size. Sound diffracts easily around corners (long wavelengths). Light diffracts less visibly (very short wavelength). Single slit and double slit diffraction patterns are classic exam problems.
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Resonance in Pipes
Pitch of open pipe: f = v/2L. Closed pipe: f = v/4L. Closed has only odd harmonics.
Resonance in Pipes
Standing waves in air columns β open vs closed pipes
Open pipe (open both ends): resonates at L = nΞ»/2. Fundamental frequency fβ = v/2L. Has all harmonics. Closed pipe (one closed end): resonates at L = nΞ»/4 (odd n only). Fundamental fβ = v/4L. Has only odd harmonics (1st, 3rd, 5th...). Flutes are open pipes, clarinets are closed.
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π Resonance in Pipes
Open vs closed pipes β fundamental frequency and harmonics?
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π Answer
Pitch of open pipe: f = v/2L. Closed pipe: f = v/4L. Closed has only odd harmonics.
Open pipe (open both ends): resonates at L = nΞ»/2. Fundamental frequency fβ = v/2L. Has all harmonics. Closed pipe (one closed end): resonates at L = nΞ»/4 (odd n only). Fundamental fβ = v/4L. Has only odd harmonics (1st, 3rd, 5th...). Flutes are open pipes, clarinets are closed.
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Wave Polarization
Polarization: transverse waves can be polarized. Sound waves (longitudinal) cannot be polarized.
Wave Polarization
Why some waves can be polarized and others cannot
Transverse waves oscillate perpendicular to travel β can be restricted to one plane (polarized). Light can be polarized by filters, reflection, or scattering. Polaroid sunglasses reduce glare by blocking horizontally polarized reflected light. Longitudinal waves (sound) oscillate parallel to travel β cannot be polarized.
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π Wave Polarization
Polarization β which waves can be polarized?
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π Answer
Polarization: transverse waves can be polarized. Sound waves (longitudinal) cannot be polarized.
Transverse waves oscillate perpendicular to travel β can be restricted to one plane (polarized). Light can be polarized by filters, reflection, or scattering. Polaroid sunglasses reduce glare by blocking horizontally polarized reflected light. Longitudinal waves (sound) oscillate parallel to travel β cannot be polarized.
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Wave Speed Equation
v = fΞ» β speed equals frequency times wavelength. Higher frequency = shorter wavelength (speed fixed in medium).
The fundamental wave equation linking speed, frequency, and wavelength
In a given medium, wave speed is fixed β so higher frequency always means shorter wavelength
v = fΞ» where v = wave speed (m/s), f = frequency (Hz), Ξ» = wavelength (m). Speed of sound in air: ~343 m/s at 20Β°C (increases with temperature). Speed of light in vacuum: c = 3Γ10βΈ m/s. In a medium: v = c/n where n is the refractive index. When a wave crosses into a new medium: frequency stays constant, speed and wavelength both change. Period T = 1/f. Angular frequency Ο = 2Οf.
v = fΞ»
Speed = frequency Γ wavelength β the fundamental wave equation
New medium
Frequency unchanged, speed changes β wavelength changes
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π Wave Speed Equation
The wave speed equation?
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π Answer
v = fΞ» β speed equals frequency times wavelength. Higher frequency = shorter wavelength (speed fixed in medium).
v = fΞ»Speed = frequency Γ wavelength β the fundamental wave equation
New mediumFrequency unchanged, speed changes β wavelength changes
T = 1/fPeriod is reciprocal of frequency
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Beat Frequency
f_beat = |fβ - fβ| β two close frequencies interfere to create a pulsing beat at their difference
Why two slightly different frequencies create a periodic rise and fall in volume
Beats are constructive and destructive interference cycling at the difference frequency
When two waves of slightly different frequencies overlap, they alternately reinforce and cancel: f_beat = |fβ β fβ|. At the beat: the waves are in phase (loud). Between beats: they are out of phase (quiet). Used for tuning instruments β when beats disappear, the two sources are at the same frequency. Faster beats = greater frequency difference. Used in ultrasound imaging (beat frequency between transmitted and reflected waves gives velocity via Doppler).
f_beat = |fβ - fβ|
Absolute difference of the two frequencies
Tuning use
Beats disappear when frequencies are equal β used to tune instruments
Fast beats
Large frequency difference. Slow beats = nearly in tune.
The full electromagnetic spectrum from lowest to highest energy
All EM waves travel at c in vacuum β only frequency and wavelength differ, determining energy E = hf
Radio waves: longest wavelength, lowest frequency, lowest energy. Microwaves: used in communication and cooking (resonates water molecules). Infrared: heat radiation, TV remotes. Visible: 400β700 nm (violet to red). Ultraviolet: causes sunburn, kills bacteria. X-rays: penetrates soft tissue, ionizing. Gamma rays: shortest wavelength, highest energy, most penetrating β from nuclear decay. Energy E = hf = hc/Ξ». Ionizing radiation: UV, X-ray, gamma (enough energy to knock electrons off atoms).
RMIVUXG
Radio β Micro β IR β Visible β UV β X-ray β Gamma
Visible
400β700 nm β violet (400) to red (700)
Ionizing
UV and above β enough energy to remove electrons from atoms
IonizingUV and above β enough energy to remove electrons from atoms
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Shock Waves and Sonic Boom
Mach number = v_source / v_sound. Mach > 1 = supersonic β shock wave β sonic boom
What happens when a source moves faster than the waves it produces
When the source outruns its own wavefronts they pile up into a cone-shaped shock wave
Mach number M = v_source / v_sound. M < 1: subsonic. M = 1: transonic (sound barrier). M > 1: supersonic β source outruns wavefronts β Mach cone forms. Half-angle of cone: sin ΞΈ = v_sound / v_source = 1/M. Sonic boom: the shock wave passing over an observer β not a one-time event but a continuous cone. Cherenkov radiation: same concept for charged particles moving faster than light in a medium β produces blue glow in nuclear reactors.
Mach 1
Source speed = sound speed β wavefronts pile up at source
Mach > 1
Supersonic β cone forms, sin ΞΈ = 1/M
Sonic boom
Continuous cone passing observer β not a single event