Propagation of Sound Waves

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Vocabulary practice flashcards covering the production, propagation, characteristics, governing equations, medium dependencies, and comparative speeds of sound waves.

26 Terms

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Sound

A form of mechanical energy produced by vibrating bodies that travels through a medium in the form of waves to produce the sensation of hearing in our ears.

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Tuning Fork

A rectangular rod of steel or aluminium bent into a U shape with a metallic stem at the bend, used to produce sound waves through the mechanical vibrations of its prongs.

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Bell Jar Experiment

A demonstration using an electric bell suspended in a glass bell jar connected to a vacuum pump, showing that sound becomes inaudible once air is completely evacuated and thus requires a material medium to propagate.

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Elasticity of the Medium

A requisite property of a medium for sound propagation that ensures displaced particles are capable of returning to their initial mean positions after being disturbed.

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Inertia of the Medium

A requisite property of a transmitting medium that enables its particles to store mechanical energy during wave propagation.

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Compression (CC)

A region in a longitudinal wave where the layers of the medium are pushed together, causing maximum density and maximum pressure.

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Rarefaction (RR)

A region in a longitudinal wave where the layers of the medium expand or separate, causing minimum density and minimum pressure.

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Longitudinal Wave

A wave in which the particles of the medium vibrate about their mean positions parallel to the direction of propagation of the wave, capable of traveling in solids, liquids, and gases.

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Transverse Wave

A wave composed of crests and troughs in which the particles of the medium vibrate perpendicular to the direction of wave propagation; it can only propagate in solids and on the surfaces of liquids.

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Crest

The position of maximum upward displacement of the particles of a medium in a transverse wave.

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Trough

The position of maximum downward displacement of the particles of a medium in a transverse wave.

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Amplitude (aa)

The maximum displacement of a particle of the medium on either side of its mean position as a wave passes through, measured in metres (m\text{m}).

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Time Period (TT)

The time taken by a particle of a medium to complete one full vibration, measured in seconds (s\text{s}).

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Frequency (ff)

The number of vibrations made by a medium particle in one second, defined by f=1Tf = \frac{1}{T}, measured in hertz (Hz\text{Hz}) or s−1\text{s}^{-1}, and determined solely by the source of the disturbance.

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Wavelength (λ\lambda)

The distance travelled by a wave during one time period (TT) of vibration, equal to the separation between two consecutive compressions, rarefactions, crests, or troughs, measured in metres (m\text{m}).

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Wave Velocity (VV)

The distance travelled by a wave per second (V=fλV = f\lambda), representing the speed at which energy is transferred through the medium, measured in m s−1\text{m\,s}^{-1}.

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Displacement-Distance Graph

A graphical representation showing the instantaneous displacement of various medium particles relative to distance along the wave's path, also termed a snapshot of a wave.

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Newton's Formula for Speed of Sound

The expression V=PρV = \sqrt{\frac{P}{\rho}} derived under the assumption that sound propagation in a gas is an isothermal process where the elasticity modulus equals pressure (E=PE = P), predicting a speed of 279.5 m s−1279.5\,\text{m\,s}^{-1} in air at N.T.P.

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Laplace's Correction

The correction to Newton's formula stating that sound travels via an adiabatic process without heat exchange (E=γPE = \gamma P), giving the formula V=γPρV = \sqrt{\frac{\gamma P}{\rho}}, yielding approximately 330.7 m s−1330.7\,\text{m\,s}^{-1} in air at N.T.P.

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Adiabatic Ratio (γ\gamma)

The ratio of the specific heat of a gas at constant pressure to that at constant volume (γ=CpCv\gamma = \frac{C_p}{C_v}), which has a value of 1.41.4 for air.

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Temperature Effect on Sound Speed

The direct proportionality of the speed of sound in a gas to the square root of absolute temperature (V∝TV \propto \sqrt{T}), increasing by approximately 0.61 m s−10.61\,\text{m\,s}^{-1} for each degree Celsius rise (Vt=V0+0.61tV_t = V_0 + 0.61t).

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Humidity Effect on Sound Speed

The increase in the speed of sound in moist air compared to dry air, caused by the lower density of water vapour (about 58\frac{5}{8} times the density of dry air at ordinary temperatures).

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Wind Effect on Sound Speed

The variation in apparent sound speed depending on wind motion, resulting in V+WV + W when traveling with the wind and V−WV - W when traveling against the wind.

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Pressure Independence of Sound Speed

The principle that changes in gas pressure do not alter the speed of sound because density varies proportionally with pressure, keeping the ratio Pρ\frac{P}{\rho} constant.

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Speed of Sound vs. Speed of Light

A physical comparison where light is a transverse electromagnetic wave traveling through a vacuum at 3×108 m s−13 \times 10^8\,\text{m\,s}^{-1}, while sound is a longitudinal mechanical wave requiring a medium and traveling at only 330 m s−1330\,\text{m\,s}^{-1} in air at 0∘C0^\circ\text{C}.

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Two-Observer Method

An experimental technique for finding the speed of sound in air by firing guns alternately between two separated stations AA and BB over a known distance dd, using V=2dt1+t2V = \frac{2d}{t_1 + t_2} to eliminate errors caused by wind flow.