Presentation is loading. Please wait.

Presentation is loading. Please wait.

Introducing Sound Waves David William D. Ecoben III-Archimedes.

Similar presentations


Presentation on theme: "Introducing Sound Waves David William D. Ecoben III-Archimedes."— Presentation transcript:

1 Introducing Sound Waves David William D. Ecoben III-Archimedes

2 The Nature of Sound  Sound travels in waves as it moves through the air or some other medium (substance)  Waves are produced by a vibrating object.  As a vibrating object moves outward, it compresses the surrounding medium, producing a region of compression called a condensation.  As the vibrating object then moves inward, the medium expands into the space formerly occupied by the object. This region of expansion is called a rarefaction.

3

4  Sound waves consist of these condensations and rarefactions.  Sound waves must travel through a medium.  Sound is called a longitudinal wave because the vibrations are in the same direction as the motion and speed of the wave.  It travels at a speed of 331 m/s in air at 0 o C.  The speed increases, at a rate of 0.6 m/s per Celsius degree.  If something moves faster than sound, it is said to be supersonic. If it travels at the speed of sound, it travels at Mach 1; three times the speed of the sound is called Mach 3.

5  Acoustics is the science of sound and of its effects on people.  Condensation is a region of compression in a sound wave.  Frequency of sound waves refers to the number of condensation or rarefactions produced by a vibrating object each second.  Decibel is the unit used to measure the intensity level of a sound. A 3000-hertz tone of zero decibels is the weakest sound that the normal human can hear.  Hertz is the unit used to measure frequency. One hertz equals one cycle (vibration) per second.  *Other terms used in the study of sound can be found in page 451.

6  The nature of a particular sound can be described in terms of  Frequency and Pitch  Intensity and loudness and  Quality

7 Frequency and Pitch  Pitch is related to its frequency. Higher frequency means higher pitch.  Frequencies of sound waves humans can hear range from about 20-20,000 hertz or cycles per second.  The loudness of sound is related to the wave’s energy or intensity.  As the frequency of sound waves increases, the wavelength decreases. Wavelength is the distance between any point on one wave and the corresponding point on the next one.

8

9

10 The Doppler Effect on Waves  The apparent change in pitch produced by moving objects is called the Doppler Effect.  Sound waves undergo the Doppler Effect. When the source of the waves moves at a constant speed relative to you, the observer, the frequency of the wave as observed by you is shifted.

11 For sound, the shifted frequency f observed, in hertz, is given by:  f observed = f source x (v source - v observer ) (v source - v sound ) Where: F source = frequency in hertz at the source of the sound V source = the speed in m/s of the source of the sound V observer = the speed in m/s of the observer, v source – v observer = the relative speed in m/s of the source with respect to the observer, and V sound = the speed of sound in m/s.

12 Example 12.5 Emergency A fire truck siren emits a sinusoidal wave with a source frequency f source of 400 Hz. The speed of sound is 340 m/s. Find the wavelength of the siren while at rest. If the truck is moving with velocity v source = 40 m/s, find the wavelength of the siren going nearer to and then away from a stationary observer.

13 Given: Source frequency f source 400 Hz Velocity of source v source 40 m/s Velocity of the observer v observer 0 Find a. Wavelength if the source is at rest b. Wavelength if the source is nearing the observer c. Wavelength if the source is going away from the observer

14  Solution:  A. When source is at rest, using the equation v = f λ  Solving for λ,  λ = v source   f source  λ = 340 m/s / 400 Hz  λ = O.85 m

15  B. In front of the siren, since the object is getting farther, then the speed of sound relative to the observer is v – v s, so  λ = (v – v source ) / f source  = (340 m/s – 40 m/s) / 400 Hz  λ = 0.75 m

16 c. Behind the siren, since the object is going nearer, then the speed of sound relative to the observer is v + v s, so λ = (v + v source ) / f source = (340 m/s + 40 m/s) / 400 Hz λ = 0.95 m

17


Download ppt "Introducing Sound Waves David William D. Ecoben III-Archimedes."

Similar presentations


Ads by Google