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Honors Physics Chapter 14

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Presentation on theme: "Honors Physics Chapter 14"— Presentation transcript:

1 Honors Physics Chapter 14
Waves and Sound Honors Physics Chapter 14

2 Definition of a wave A disturbance that propagates from 1 place to another. Characterized by a large transfer of energy without a large transfer of medium

3 Types of waves Mechanical waves: require a medium (air, water, ropes) to travel Electromagnetic waves: do not require a medium to travel (light, radio) Matter waves: produced by electrons and particles

4 Mechanical Waves Transverse: the displacement of the individual particles is perpendicular to the direction of propagation.

5 Mechanical Waves Longitudinal: The displacement of the individual particles is parallel to the direction of propagation.

6 Mechanical Waves Surface waves: the displacement of individual particles is circular (result of both transverse and longitudinal motion)

7 Waves in motion Longitudinal and Transverse Wave Motion

8 Properties of waves Amplitude (A): the maximum displacement from equilibrium position, measured in meters. Wavelength ( λ): the distance between 2 particles that are in phase with each other, measured in meters.

9 Wave diagram

10 Properties of waves 3. Frequency (f): number of complete waves that pass a point in one second, measured in 1/seconds or Hertz (Hz) 4. Period (T): the time it takes for one complete wave to pass a given point, measured in seconds.

11 Properties of waves Velocity of propagation (v): horizontal speed of a point on a wave as it propagates, measured in m/s.

12 Relationships/equations
T =1/ f or f = 1/T v = f × λ

13 Phase In-phase: when waves are synchronized (crest meets crest)
Out-of-phase: waves are not synchronized Opposite phase (180º out-of-phase): crest meets trough

14 Reflections Fixed End: Explanation Animation Open End: Between different mediums scroll down (What do you notice about the phases? Transmitted? Reflected?)

15 Principle of Superposition
Occurs when two waves travel through the same medium at the same time. Each wave affects the medium independently. The displacement of the medium is the algebraic sum of the displacements. Animation (scroll down)

16 Interference Constructive: occurs when wave displacements are in the same direction (in-phase) Destructive: occurs when wave displacement are in different directions (out-of-phase) animation

17 What is Sound? Longitudinal Mechanical Rarefaction: low air pressure
Compression: high air pressure module animation What is Sound?

18 Speed of sound Depends on… Temperature V air = 331m/s +(0.6 m/s/ºC)*T
Density/kind of medium Gases <liquids<solids Chart of speeds

19 Speed of sound

20 Pitch How we perceive variations in frequency Audible range 20-20,000 Hz (listen) Most sensitive to 1,000 to 5,000Hz Loudness can distort our perception of pitch (listen tape) module

21 Doppler Effect Variation in the frequency of sound due to the relative motion of the sound source or the listener. Animation1 Picture of a sonic boom Video of sonic boom Space shuttle breaking sound barrier

22 Doppler Effect Results
As an moving sound source approaches a listener the frequency (pitch) increase. As a moving sound source passes by a listener the frequency (pitch) decreases. *Same effect if sound source is stationary and listener is moving.

23 Calculating Frequency change
f’ = f (v ± vR / v± vs) f’ = new frequency f = original frequency of source sound v: velocity of sound vR: velocity of receiver vs: velocity of source

24 Loudness How we perceive variations in amplitude and intensity. Module In general, sound waves of higher intensity sound louder but we are not equally sensitive to all frequencies.

25 Sound Intensity The amount of energy that passes through a given area in a given time. I=P/A P=power (watts) A = area (m2) I = intensity (W / m2) Directly proportional to the square of the amplitude. Inversely proportional to the square of the distance from the source.

26 Relative Intensity Logarithmic scale used to indicate the intensity level of a sound. Measured in decibels or dB β= 10 log (I / Io) Io =1×10-12 W/m2 (intensity of the faintest sound that can be heard) I = intensity of sound in W/m2

27 How loud is a decibel? Threshold of hearing( Io )= 0dB (air pressure 2×10-5 Pa) Threshold of pain = 120 dB (air pressure = 20 Pa) We perceive a 10 dB increase as twice as loud. Every 20 decibels air pressure increases 10 times Table of sound levels

28 Resonance Causing the vibration of an object by the influence of another vibrating body. Must match the natural frequency of vibration of the object Whole-number multiple of the natural frequency work too. DEMO (wood blocks)

29 Standing waves Caused by the interference of reflected waves with incident waves from the source. Nodes: pts of no displacement Antinodes: pts of maximum displacement Animation applet

30 Vibrating Columns of Air
Column will emit a sound when the air inside achieves resonance. DEMO (cardboard moose call) Frequency of vibration depend on Length of column Type of column Open end Closed end

31 Fundamentals and Harmonics
Fundamental Frequency: lowest frequency of vibration Harmonics: whole number multiples of the fundamental Note: the fundamental frequency is the 1st harmonic. Animation

32 Closed (at one end) pipe
The standing wave created has Node at closed-end Antinode at open-end A N

33 Calculations for closed pipe
Fundamental frequency f1= v /4L (L=length of air column) Harmonics fn = nf1 (n=1,3,5,…) λ =4L/n Note: only ODD harmonics are produced Animation

34 Open pipe The standing wave created has Antinode at both ends A A

35 Calculations for open pipe
Fundamental frequency f1= v /2L (L=length of air column) Harmonics fn = nf1 (n=1,2,3,…) λ =2L/n Note: ALL harmonics are produced animation

36 Frequency Light Sound (listen) BACK


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