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This chapter explores the fundamentals of waves, including different types, properties like amplitude and wavelength, speed, and the phenomenon of interference. It also discusses standing waves and their characteristics.
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Chapter 17 Waves
Wave Motion • Fundamental to physics (as important as particles) • A wave is the motion of a disturbance • All waves carry energy and momentum • Mechanical waves require • Some source of disturbance • A medium that can be disturbed • Some physical connection between or mechanism though which adjacent portions of the medium influence each other
Types of Waves – Traveling Waves • Flip one end of a long rope that is under tension and fixed at one end • The pulse travels to the right with a definite speed • A disturbance of this type is called a traveling wave
Types of Waves – Transverse • In a transverse wave, each element that is disturbed moves in a direction perpendicular to the wave motion
Types of Waves – Longitudinal • In a longitudinal wave, the elements of the medium undergo displacements parallel to the motion of the wave • A longitudinal wave is also called a compression wave
Other Types of Waves • Waves may be a combination of transverse and longitudinal • Mainly consider periodic sinusoidal waves
Waveform – A Picture of a Wave • The brown curve is a “snapshot” of the wave at some instant in time • The blue curve is later in time • The high points are crests of the wave • The low points are troughs of the wave
Longitudinal Wave Represented as a Sine Curve • A longitudinal wave can also be represented as a sine curve • Compressions correspond to crests and stretches correspond to troughs • Also called density waves or pressure waves
Amplitude and Wavelength • Amplitude is the maximum displacement of string above the equilibrium position • Wavelength, λ, is the distance between two successive points that behave identically
Speed of a Wave • v = ƒ λ • Is derived from the basic speed equation of distance/time • This is a general equation that can be applied to many types of waves
Speed of a Wave on a String • The speed of wave on a stretched rope under some tension, F • m is called the linear density • The speed depends only upon the properties of the medium through which the disturbance travels
Example String vibrates at 10 hz and a snapshot. Determine wavelength, period, amplitude, speed.
Example Mass and length of the string are 0.9 kg and 8 m. What is the speed of wave on the string?
Wave fronts & rays • Wave fronts – locate crests of waves • Ripples from a pebble dropping in a pond • concentric arcs • The distance between successive wave fronts is the wavelength • Rays are the radial lines pointing out from the source and perpendicular to the wave fronts
Plane Wave • Far away from the source, the wave fronts are nearly parallel planes • The rays are nearly parallel lines • A small segment of the wave front is approximately a plane wave
Reflection of Waves • Waves reflect when they hit boundaries • Fixed end: wave inverts upon reflection • Free end: no inversion
Superposition Principle • Two traveling waves can meet and pass through each other without being destroyed or even altered • Waves obey the Superposition Principle • If two or more traveling waves are moving through a medium, the resulting wave is found by adding together the displacements of the individual waves point by point • Actually only true for waves with small amplitudes
Constructive Interference • Two waves, a and b, have the same frequency and amplitude • Are in phase • The combined wave, c, has the same frequency and a greater amplitude
Constructive Interference in a String • Two pulses are traveling in opposite directions • The net displacement when they overlap is the sum of the displacements of the pulses • Note that the pulses are unchanged after the interference
Destructive Interference • Two waves, a and b, have the same amplitude and frequency • They are 180° out of phase • When they combine, the waveforms cancel
Destructive Interference in a String • Two pulses are traveling in opposite directions • The net displacement when they overlap is decreased since the displacements of the pulses subtract • Note that the pulses are unchanged after the interference
Standing Waves • When a traveling wave reflects back on itself, it creates traveling waves in both directions • The wave and its reflection interfere according to the superposition principle • With exactly the right frequency, the wave will appear to stand still • This is called a standing wave
Standing Waves, cont • A node occurs where the two traveling waves have the same magnitude of displacement, but the displacements are in opposite directions • Net displacement is zero at that point • The distance between two nodes is ½λ • An antinode occurs where the standing wave vibrates at maximum amplitude • The distance between two antinodes is ½λ • Distance between node and antinode λ/4
Standing Waves on a String • Nodes must occur at the ends of the string because these points are fixed
Standing Waves, cont. • The pink arrows indicate the direction of motion of the parts of the string • All points on the string oscillate together vertically with the same frequency, but different points have different amplitudes of motion
Resonance • Can have resonance in strings (these are actually standing waves) • Amplitude increases • How to determine resonance frequencies?
Standing Waves on a String, final • The lowest frequency of vibration (b) is called the fundamental frequency
Standing Waves on a String – Frequencies • ƒ1, ƒ2, ƒ3 form a harmonic series • ƒ1 is the fundamental and also the first harmonic • ƒ2 is the second harmonic (1st overtone) • Waves in the string that are not in the harmonic series are quickly damped out • In effect, when the string is disturbed, it “selects” the standing wave frequencies
Example A guitar has 0.6 m long string. Wave speed on the string is 420 m/s. What are the frequencies of the first few harmonics?
Example String 80 cm long is driven with frequency of 120 Hz when both ends fixed. There are 4 nodes in the middle of the string. Find speed of wave on string?
Producing a Sound Wave • Sound waves are longitudinal waves traveling through a medium • A tuning fork can be used as an example of producing a sound wave
Using a Tuning Fork to Produce a Sound Wave • A tuning fork will produce a pure musical note • As the tines vibrate, they disturb the air near them • As the tine swings to the right, it forces the air molecules near it closer together • This produces a high density area in the air • This is an area of compression
Using a Tuning Fork, cont. • As the tine moves toward the left, the air molecules to the right of the tine spread out • This produces an area of low density • This area is called a rarefaction
Using a Tuning Fork, final • As the tuning fork continues to vibrate, a succession of compressions and rarefactions spread out from the fork • A sinusoidal curve can be used to represent the longitudinal wave • Crests correspond to compressions and troughs to rarefactions
Categories of Sound Waves • Audible waves • Lay within the normal range of hearing of the human ear • Normally between 20 Hz to 20,000 Hz • Infrasonic waves • Frequencies are below the audible range • Earthquakes are an example • Ultrasonic waves • Frequencies are above the audible range • Dog whistles are an example
Applications of Ultrasound • Can be used to produce images of small objects • Widely used as a diagnostic and treatment tool in medicine • Ultrasounds to observe babies in the womb • Cavitron Ultrasonic Surgical Aspirator (CUSA) used to surgically remove brain tumors • Ultrasonic ranging unit for cameras
Speed of Sound, General • The speed of sound is higher in solids than in gases • The speed is slower in liquids than in solids
Speed of Sound in Air • 331 m/s is the speed of sound at 0°C and 1 atm • Changes with temperature • T in °C • At 20 °C, 343 m/s • In other substances in He: 1000 m/s in Water: 1500 m/s in Al: 5000 m/s
Standing Waves in Air Columns • If one end of the air column is closed, a node must exist at this end since the movement of the air is restricted • If the end is open, the elements of the air have complete freedom of movement and an antinode exists
Resonance in Air Column Open at Both Ends • In a pipe open at both ends, the natural frequency of vibration forms a series whose harmonics are equal to integral multiples of the fundamental frequency
Tube Closed at One End Closed pipe
Resonance in an Air Column Closed at One End • The closed end must be a node • The open end is an antinode • There are no even multiples of the fundamental harmonic
Example An open organ pipe has a fundamental frequency of 660 Hz at 0 C and 1 atm. • Frequency of 2nd overtone? • Fundamental at 20 C? • Replacing air with He?