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Published byDaniel Perkins Modified over 9 years ago
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Sound
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Sound Waves Sound waves are longitudinal waves. The source of a sound wave is a vibrating object. Only certain wavelengths of longitudinal waves in the air can be detected as sound.
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Sound Waves Sound waves require matter in order to propagate. They cannot travel in a vacuum The speed of sound is different in different materials. The speed of sound is also somewhat dependent on temperature.
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Speed of Sound Air (room temp) – 343 m/s Air (0° C) – 331 m/s Helium – 1005 m/s Water – 1440 m/s Steel – about 5000 m/s Concrete – about 3000 m/s
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Loudness Loudness is related to intensity. Loudness itself is not a measurable physical quantity. It depends on the listener. Intensity is measurable, however.
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Loudness Sound intensity levels are usually given on a logarithmic scale. The unit on this scale is the decibel (dB) β = 10 log (I/I ₀ ) β = sound level (in dB) I = sound intensity I ₀ = base sound level
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Loudness The base sound level used (I ₀ ) is usually what is know as the “threshold of hearing” This is the minimum intensity that is audible to a good ear. 1.0 x 10ֿ¹² W/m²
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Sound Intensities Threshold of hearing – 0 dB Whisper – 20 dB Talk, at 50 cm – 65 dB Busy street traffic – 70 dB Loud rock concert – 120 dB Jet plane at 30 m – 140 dB
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Pitch Pitch is related to frequency of a sound wave. A high pitch corresponds to a high frequency. The audible range is the range of frequencies that a normal person can hear.
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Pitch Frequencies between 20 Hz and 20,000 Hz are audible. The threshold of hearing varies for different frequencies. It is easiest to hear sounds between 2000 and 5000 Hz.
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Pitch Frequencies too high to hear are ultrasonic. Some animals can perceive sounds up to 100,000 Hz (bats) Frequencies too low to hear are infrasonic.
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Beats
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Beats Occurs due to interference between two sound waves that are close in frequency. The sound level rises and falls as time passes. This regular change in intensity is a beat.
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Doppler Effect The Doppler Effect is the apparent change in frequency of a wave due to relative motion between the observer and the sound source. Has many uses.
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