Notes for Hw 3

SOUND ENERGY

HOW DOES SOUND ENERGY HELP US HEAR?

  • An object vibrates, causing a disturbance in the surrounding air creating sound.

  • Movement in air particles occurs, generating sound waves associated with the vibrations.

  • As a result, sound waves begin to propagate through the medium.

PITCH AND VOLUME

  • Pitch refers to how high or low a sound is.

    • Determined by the frequency of the sound waves; higher frequency corresponds to a higher pitch.

  • Volume signifies how loud or soft a sound is.

    • Influenced by the amplitude of the sound waves; higher amplitude yields a louder sound.

  • Low frequency notes: Correspond to slower vibrations.

  • High frequency notes: Correspond to faster vibrations.

    • Example: Higher frequency ($f$) equals higher pitch, higher amplitude ($A$) equals louder sound.

PROPERTIES OF SOUND WAVES

1. WAVE STRUCTURE

  • Rarefactions and Compressions:

    • Rarefactions are regions where particles are spread apart.

    • Compressions are regions where particles are close together.

  • Direction of Sound Wave: Illustrates the path that sound takes as it propagates.

2. CREST, TROUGH, AND AMPLITUDE

  • Crest: The highest point of the wave.

  • Trough: The lowest point of the wave.

  • Amplitude: The height of the wave from the equilibrium position to the crest (or trough), indicating the energy of the wave.

  • Wavelength ($ ext{λ}$): Distance between consecutive crests (or troughs).

SOUND WAVES AND VELOCITY

EQUATION OF SOUND WAVE SPEED

  • The formula for sound velocity is denoted by:
    D = R imes T
    where:

    • D = distance (in meters, m) traveled by the wave.

    • R = rate or speed of the wave.

    • T = time (in seconds).

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Wave Speed Equation
  • V = f imes ext{λ} where:

    • V = wave speed (m/s),

    • f = frequency (Hz),

    • ext{λ} = wavelength (m).

FACTORS AFFECTING SOUND SPEED

  • Temperature of the medium: Sound travels faster in warm air than in cold air; specific speeds are approximated as follows:

    • Sound Speed in Air (0°C): 331 m/s

    • Sound Speed in Air (20°C): 344 m/s

  • Medium Density: Greater density slows sound down (kg/m³).

  • Bulk Modulus: Indicates how resistant a material is to compression; higher bulk modulus equates to faster sound speed.

  • Example speed values for various materials (speed in m/s):

    • Air (0°C): 331

    • Air (20°C): 344

    • Helium (20°C): 999

    • Hydrogen (20°C): 1330

    • Water (0°C, liquid): 1400

    • Water (20°C): 1480

    • Aluminium: 6420

    • Steel: 5940

    • Lead: 1960

LOUDNESS VS INTENSITY

1. LOUDNESS

  • Definition: Perception of the sound volume by the ear.

    • Measured in decibels (dB) or bels (B).

    • Depends on the sensitivity of the ear, varying from person to person.

2. INTENSITY OF SOUND

  • Definition: The power of the wave transmitted per unit area.

    • Measured in units of watts per square meter (W/m²).

    • Intensity increases with the increasing amplitude of the sound wave.

  • Relationship:

  • Intensity ($I$) is given by:
    I = rac{P}{A}
    where:

    • P = Power (in watts), A = Area (in square meters).

COMPARATIVE ANALYSIS

  • Loudness is expressed on a logarithmic scale while intensity is typically represented on a linear scale.

    • Consequentially, doubling the intensity does not equate to it feeling twice as loud to the ear.

NOISE LEVEL DECIBEL CHART

  • Specific sound levels and associated risks:

    • 150 dB: Jet Plane, Explosion – High Risk, Hearing damage.

    • 130 dB: Formula 1 – High Noise Level, mandatory protection.

    • 110 dB: Airplane Taking Off, Jackhammer – Protection advised.

    • 100 dB: Loud environments like concert or ambulance sirens – Warning for hearing damage.

    • 85 dB: Drilling or sanding; necessary precautions advised.

    • 70 dB: Office sounds, safe listening level.

    • 60 dB: Conversations; considered normal levels.

  • Human hearing range: 20 Hz to 20,000 Hz.

    • Frequency increases (+f) correlates with pitch.

SOUND INTENSITY AND ENERGY TRANSPORT

  • Sound waves are energy transporters without the transportation of mass.

    • Intensity is a measure of the power transmitted by a wave per area.

  • Intensity Formula:
    I = rac{P}{A}
    where:

    • I = Intensity (W/m²), P = Power, A = Area.

  • Sound intensity decreases inversely with the square of distance from the source:
    I(r) = rac{P}{4πr^2}

  • Area of dispersion: Energy spreads uniformly in all directions from the sound source.

MODES OF VIBRATION OF STANDING WAVES

  • The modes of vibration in standing waves are based on the harmonic number denoted as: f_n = n rac{v}{2L} where:

    • n = harmonic number

    • L = length of the vibrating string

HARMONICS EXAMPLES
  • Example harmonic numbers (1 through 5 for a vibrating string):

    • 1st harmonic (fundamental): Frequency f_1 = rac{v}{2L}

    • 2nd harmonic (1st overtone): Frequency f_2 = rac{v}{L}

  • Nodes and Antinodes: The number of nodes present determines the mode of vibration

    • ext{Number of nodes} = n + 1

STRING INSTRUMENTS

GENERAL COMMENTS

  • Vibrations of strings create standing waves which determine the sound produced:

    • Fundamental frequency depends upon the tension, length, and linear mass density of the string.

  • Tension: Changes the pitch while length and mass typically remain constant.

  • Timbre is influenced by the harmonics created which result from how the string is excited (plucked, bowed, struck etc.).

  • Various string instruments include:

    • Violin, Guitar, Cello, Ukrainian Bandur, etc.

STANDING WAVES ON STRINGS

FORMULAE

  • Wave Speed calculation depends on tension and mass:
    V = rac{F_T}{ ext{m}}

    • where:

    • F_T = tension force (N),

    • m = mass (kg).

  • The governing principles for standing waves ensure that various harmonics produce different sounds depending on instrument design and mechanics.

  • Please note all content covers essential aspects related to sound energy and how it translates into hearing phenomena, properties of sound waves, and their applications in real-world contexts like music and environmental science.