LECTURE 9 Ch 16.7 BEATS Ch Doppler Effect

Slides:



Advertisements
Similar presentations
Chapter 12 Sound. What is sound? Sound is a compressional wave which travels through the air through a series of compressions and rarefactions.
Advertisements

Waves_04 SOUND WAVES flute clarinet click for sounds.
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley Wave interference, boundaries, and superposition Waves in motion from one.
SOUND WAVES Sound is a longitudinal wave produced by a vibration that travels away from the source through solids, liquids, or gases, but not through a.
Chapter 14 Sound.
Sound Waves Physics Chapter 13 Section 1. I. Production of sound waves Produced by an object vibrating Produced by an object vibrating -ex. Tuning fork.
Phys 250 Ch15 p1 Chapter 15: Waves and Sound Example: pulse on a string speed of pulse = wave speed = v depends upon tension T and inertia (mass per length.
Chapter 15. Properties of Sound Properties of Sound Waves Sound is a compression wave in any material medium oscillating within the frequency range of.
Chapter 14 Sound AP Physics B Lecture Notes.
Cutnell/Johnson Physics 8th edition Reading Quiz Questions
Sound waves.
Review: Oscillations and Waves LECTURE 12. Identify  Setup  Execute  Evaluate IDENTIFY Identify what the question asking Identify the known and unknown.
Lecture 1 – Waves & Sound c) Sound.
PHY 102: Waves & Quanta Topic 5 Sound John Cockburn Room E15)
Dr. Jie ZouPHY Chapter 17 Sound Waves (cont.)
Halliday/Resnick/Walker Fundamentals of Physics 8th edition
SMDEP Physics Waves: Standing Waves, Sound Waves Webpage updated:
Bell Work: Test Review 1. What is the range of human hearing?
University Physics: Waves and Electricity Ch17. Longitudinal Waves Lecture 5 Dr.-Ing. Erwin Sitompul
SOUND A vibrating object, such as your voice box, stereo speakers, guitar strings, etc., creates longitudinal waves in the medium around it. When these.
1© Manhattan Press (H.K.) Ltd. Source moving Observer moving Observer moving 11.5 Doppler effect Both source and observer moving Both source and observer.
A 100-m long high-voltage cable is suspended between two towers
Sound. Characteristics of Sound Mathematical Representation of Longitudinal Waves Intensity of Sound: Decibels Sources of Sound: Vibrating Strings and.
Sound A Mechanical wave. The Nature of a Sound Wave Sound originates when a body moves back and forth rapidly enough to send a coursing wave through the.
Waves and Sound Ch
Sound Sound is a longitudinal wave that travels through a medium. The speed of sound depends on the properties of the medium. It travels faster in a.
MECHANICAL WAVES WAVE PROPERTIES SOUND…“WHAT?”
Mechanical Waves & Sound. Wave Motion Waves are caused by.
Sound Waves Sound waves are divided into three categories that cover different frequency ranges Audible waves lie within the range of sensitivity of the.
Chapter 13 - Sound 13.1 Sound Waves.
Sound Review.
Reflection & Transmission
Wave Motion. Wave Types Longitudinal –Motion parallel to energy transport Transverse –Motion perpendicular to energy transport.
R. Field 11/26/2013 University of Florida PHY 2053Page 1 Sound Waves: Doppler Effect Doppler Shift: If either the detector or the source of sound is moving,
Chapter 14 Sound. Sound waves Sound – longitudinal waves in a substance (air, water, metal, etc.) with frequencies detectable by human ears (between ~
Chapter 17 Sound Waves: part two HW 2 (problems): 17.22, 17.35, 17.48, 17.58, 17.64, 34.4, 34.7, Due Friday, Sept. 11.
Chapter 14 Sound. Characteristics of sound 2 A special and important type of mechanical wave Speed of sound: Loudness: related to the energy of sound.
A longitudinal wave is: 1.A wave where the particle oscillation is perpendicular to the direction of wave motion 2.A wave where the particle oscillation.
Sound Waves  Sound is a longitudinal wave  It requires a medium to convey it, e.g. a gas, liquid, or solid  In a gas, the amplitude of the sound wave.
CHAPTER 14 Sound Doppler Effect A train passes by you with its whistle/horn blowing. You hear one pitch (tone) as the train is coming towards you and a.
Physics I Honors 1 Waves and Sound Intensity Doppler Effect.
Sound Sound waves are –Longitudinal –Pressure Waves Infrasonic – less than 20 Hz Audible – between 20 and 20,000 Hz Ultrasonic – greater than 20,000 Hz.
Sound Bites. Basics Sound is a mechanical, longitudinal wave. The medium usually associated with sound is air, but sound can travel through both liquids.
1 General Doppler Formula (Serway convention) f s = frequency emitted by source v S =Velocity of source f L = frequency received by listener v L =Velocity.
Sect. 12-6: Sound Wave Interference & Beats Like any other waves, sound waves can interfere with each other. Example Can lead to beats.
14-6 The Doppler Effect The Doppler effect is the change in pitch of a sound when the source and observer are moving with respect to each other. When an.
Harmonics. Each instrument has a mixture of harmonics at varying intensities Principle of superposition Periodics- Repeating patterns of waveforms.
Light & Sound BRHS- Physics Electromagnetic Radiation Energy that has properties of both particles and waves Particles – have mass and occupy space.
 For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o
1 Wave Interference: Beats 2 Beats Previously we considered two interfering waves with the same . Now consider two different frequencies. When waves.
Wave Interference For complete destructive interference to occur, two pulses must have: the same ____________________ and equal magnitude but opposite.
Beats AP Physics 1.
Chapter 12 Sound Producing a Sound Wave Characteristics of Sound Waves The Speed of Sound Spherical and Plane Waves The.
Chapter 15 Properties of Sound Pitch and Loudness Sound Intensity Level Doppler Effect.
Wave Motion Types of mechanical waves  Mechanical waves are disturbances that travel through some material or substance called medium for the waves. travel.
Sound Waves March 22-23, The nature of sound What is a tuning fork? How are they used? How do we know that sound is a wave? Visualizing sound waves.
AP PHYSICS 1 Sound Loudness Intensity and Doppler
Today (Finish Chapter 13, Sound)  Temperature and Heat Concepts Tomorrow (Start Chapter 14)  Standing Waves  Beats  Doppler Effect  Example Problems.
Chapter Summary 15.1 Properties and Detection of Sound
The Doppler Effect THE LAST LECTURE.
Section 15.7 The Doppler Effect and Shock Waves (cont.)
University Physics: Waves and Electricity
Wave interference, boundaries, and superposition
Doppler Effect Doppler Effect – The apparent change in frequency of a wave due to the motion of the source and/or the observer Stationary Source – Moving.
Sound.
Waves & Sound A. Waves 1. The nature of waves
University Physics: Waves and Electricity
University Physics: Waves and Electricity
LECTURE 9 Ch 16.7 BEATS Ch Doppler Effect
Sound, Decibels, Doppler Effect
Presentation transcript:

LECTURE 9 Ch 16.7 BEATS Ch 115.7 Doppler Effect Loud-soft-loud modulations of intensity are produced when waves of slightly different frequencies are superimposed. The beat frequency is equal to the difference frequency fbeat = | f1 - f2| 1 beat Used to tune musical instruments to same pitch CP 52

Beats two interfering sound waves can make beat Two waves with different frequency create a beat because of interference between them. The beat frequency is the difference of the two frequencies.

frequency of pulses is | f1-f2 | BEATS Superimpose oscillations of equal amplitude, but different frequencies Modulation of amplitude Oscillation at the average frequency frequency of pulses is | f1-f2 | CP 527

BEATS – interference in time Consider two sound sources producing audible sinusoidal waves at slightly different frequencies f1 and f2. What will a person hear? How can a piano tuner use beats in tuning a piano? If the two waves at first are in phase they will interfere constructively and a large amplitude resultant wave occurs which will give a loud sound. As time passes, the two waves become progressively out of phase until they interfere destructively and it will be very quite. The waves then gradually become in phase again and the pattern repeats itself. The resultant waveform shows rapid fluctuations but with an envelope that various slowly. The frequency of the rapid fluctuations is the average frequencies = The frequency of the slowly varying envelope = Since the envelope has two extreme values in a cycle, we hear a loud sound twice in one cycle since the ear is sensitive to the square of the wave amplitude. The beat frequency is CP 527

f1 = 100 Hz f2 = 104 Hz frapid = 102 Hz Trapid = 9.8 ms fbeat = 4 Hz Tbeat = 0.25 s (loud pulsation every 0.25 s) CP 527

f1 = 100 Hz f2 = 110 Hz frapid = 105 Hz Trapid = 9.5 ms fbeat = 10 Hz Tbeat = 0.1 s (loud pulsation every 0.1 s) CP 527

f1 = 100 Hz f2 = 120 Hz frapid = 110 Hz Trapid = 9.1 ms fbeat = 20 Hz Tbeat = 0.05 s (loud pulsation every 0.05 s) CP 527

What is the physics of this image? CP 495

DOPPLER EFFECT - motion related frequency changes Doppler 1842, Buys Ballot 1845 - trumpeters on railway carriage Source (s) Observer (o) formula different to textbook Applications: police microwave speed units, speed of a tennis ball, speed of blood flowing through an artery, heart beat of a developing fetous, burglar alarms, sonar – ships & submarines to detect submerged objects, detecting distance planets, observing the motion of oscillating stars. note: formula is very different to textbook CP 495

Doppler Effect v =  f Consider source of sound at frequency fs, moving speed vs, observer at rest (vo = 0) Speed of sound v What is frequency fo heard by observer? On right - source approaching source catching up on waves wavelength reduced frequency increased On left - source receding source moving away from waves wavelength increased frequency reduced CP 495

CP 495

source vs observer vo observed frequency fo stationary = fs receding < fs approaching > fs ? CP 595

Shock Waves – supersonic waves CP 506

Shock Waves – supersonic waves CP 506

Problem 9.1 A train whistle is blown by the driver who hears the sound at 650 Hz. If the train is heading towards a station at 20.0 m.s-1, what will the whistle sound like to a waiting commuter? Take the speed of sound to be 340 m.s-1. [Ans: 691 Hz]

Problem 9.2 The speed of blood in the aorta is normally about 0.3000 m.s-1. What beat frequency would you expect if 4.000 MHz ultrasound waves were directed along the blood flow and reflected from the end of red blood cells? Assume that the sound waves travel through the blood with a velocity of 1540 m.s-1.

Solution 9.2 I S E E Doppler Effect Beats

Blood is moving away from source  observer moving away from source  fo < fs Wave reflected off red blood cells  source moving away from observer  fo < fs Beat frequency = | 4.00 – 3.998442| 106 Hz = 1558 Hz In this type of calculation you must keep extra significant figures.

An ambulance travels down a highway at a speed of 33.5 m.s-1, its Problem 8.3 An ambulance travels down a highway at a speed of 33.5 m.s-1, its siren emitting sound at a frequency of 4.00x102 Hz. What frequency is heard by a passenger in a car traveling at 24.6 m.s-1 in the opposite direction as the car and ambulance: (a) approach each other and (b) pass and move away from each others? Speed of sound in air is 345 m.s-1. Solution (a) (b)