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Ch 20 SOUND

Ch 20 SOUND. Sound is a compression wave in an elastic medium. These can include solids, liquids and gases or a plasma. Human hearing can detect sound waves with frequencies between 20 Hz and 20,000Hz (20kHz).

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Ch 20 SOUND

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  1. Ch 20 SOUND • Sound is a compression wave in an elastic medium. These can include solids, liquids and gases or a plasma.

  2. Human hearing can detect sound waves with frequencies between 20 Hz and 20,000Hz (20kHz). Frequencies below20Hz are called infrasonic. They are inaudible to human hearing. (We can’t hear them!)

  3. Frequencies above 20,000Hz are called ultrasonic. They are also inaudible to human hearing. (Again, we can’t hear them, but some animal can!)

  4. Media That Transmit Sound • Any elastic material can transmit sound. • Steel is a very good conductor of sound. • Water is not as good a conductor as steel, but is better than air. • Air is a poor conductor of sound

  5. Speed of Sound • Sound waves will have different speeds in different media. The speed also varies with temperature. • Sound travels 15 times faster in steel than in air, and it travels 4 times faster in water than in air. • Sound travels at about 330 m/s in air at 0 oC and 340 m/s in air at 20 oC.

  6. Reflection of Sound • Echo - The reflection of sound. • E.G. Singing in the shower. • Sound reflects off of a smooth surface at the same angle at which it is incident. • (i.e. The angle of reflection equals the angle of incidence.)

  7. Refraction • Refraction is the bending of the sound wave. Sound waves bend when parts of the wave front travel at different speeds. • This occurs when there are: • Uneven Winds. • Uneven Temperatures. • The speed of sound is slightly faster in warm air than in cool air.

  8. Energy in Sound Waves • Sound generally transmits only a small amount of energy. • (10,000,000 people talking at the same time = energy needed to light a common flashlight). • Sound energy dissipates to thermal energy (heat) while sound travels through air.

  9. High frequency sound dissipates to thermal energy more rapidly than low frequency sound. • Hence, low frequency sound has a greater range in air than high frequency sound. (Fog horns typically produce low frequency sound, but have a long range)

  10. Forced Vibrations • The setting up of vibrations in an object by a vibrating force. Examples: 1) Sounding board of a musical instrument. 2) The box of a music box.

  11. Natural Frequency A frequency at which an elastic object naturally tends to vibrate if it is disturbed and the disturbing force is removed. The natural frequency of an object depends on such factors as the elasticity and shape of the object.

  12. When the frequency of a forced vibration (driving frequency) matches the object’s natural frequency, a dramatic increase in amplitude occurs. This is known as resonance. Example: Pushing someone on a swing.

  13. Resonance • The response of a body when a forcing frequency matches its natural frequency.

  14. Sound Interference • Sound waves can interfere with each other just like transverse waves interfere. Transverse Wave Interference + Longitudinal (Sound) wave interference +

  15. Beats • When two tones of slightly different frequencies are sounded together, a fluctuation of the loudness of the combined sounds is heard. • Alternating loud and faint sound can be heard. This periodic variation in loudness is called beats.

  16. Beats f1 f2 fbeat= |f1 - f2|

  17. Standing Waves on a String STANDING WAVES ON A STRING SUPERPOSITION OF WAVES

  18. Parts of a Standing Wave on a String Fundamental (1st harmonic) NODES 2nd harmonic (1st overtone) Antinodes 3rd harmonic (2nd overtone)

  19. Fundamental (1st harmonic) L = /2 2nd harmonic (1st overtone) L = 

  20. Tuning fork L1= /4 Standing Waves in an air column – open tube at one end Fundamental (first harmonic)

  21. L2= 3/4 Third harmonic- open at one end

  22. End of Chapter 19

  23. Simulations

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