Physics Acoustics for Musicians

Slides:



Advertisements
Similar presentations
SOUND PRESSURE, POWER AND LOUDNESS MUSICAL ACOUSTICS Science of Sound Chapter 6.
Advertisements

PHY 102: Waves & Quanta Topic 3 Energy in wave motion
Hearing and Deafness 2. Ear as a frequency analyzer Chris Darwin.
SOUND ENERGY, INTENSITY AND POWER The acoustic power of a sound source is the amount of sound energy produced by a source per second. Acoustic power.
Physics 1251 The Science and Technology of Musical Sound Unit 2 Session 13 MWF Sound Intensity Level and dB Unit 2 Session 13 MWF Sound Intensity Level.
Chapter 12 SOUND.
Loudness Physics of Music PHY103 experiments: mix at different volumes
The Doppler Effect A source emits a sound of constant frequency. If the apparent frequency of the source is increased which of the following is true? A.
Music Physics 202 Professor Lee Carkner Lecture 10.
Chapter 16: Sound 16-3 Intensity of Sound: Decibels
PH 105 Dr. Cecilia Vogel Lecture 10. OUTLINE  Subjective loudness  Masking  Pitch  logarithmic  critical bands  Timbre  waveforms.
HEARING MUSICAL ACOUSTICS Science of Sound Chapter 5.
Reading Assignment! We’ll discuss the chapter by Gregory in your book on Friday of next week.
Music Physics 202 Professor Vogel (Professor Carkner’s notes, ed) Lecture 8.
Lighting and Acoustics Arch 353 Dr. Abdelrahman Elbakheit References اسس الانارة المعمارية, أستاذ الدكتور محمد عبد الفتاح عبيد.1 2. Architectural Lighting,
PH 105 Dr. Cecilia Vogel Lecture 8. OUTLINE  Exam #1  Hearing  subjective qualities of sound  the ear  intensity vs pressure  pressure and frequency.
PH 105 Dr. Cecilia Vogel Lecture 9. OUTLINE  Finish ear/hearing  Source power level  Sound loudness  sound intensity level  sound pressure level.
EE2F1 Speech & Audio Technology Sept. 26, 2002 SLIDE 1 THE UNIVERSITY OF BIRMINGHAM ELECTRONIC, ELECTRICAL & COMPUTER ENGINEERING Digital Systems & Vision.
Chapter 6: The Human Ear and Voice
L6 and L7 Sound Intensity, Sound Level/Loudness (Decibels), The Ear.
Chapter 16 – Waves and Sound
Acoustics and Noise. Physics of Sound Sound is a response to pressure waves  = c = ° C in air Amplitude: Pressure [N/m 2 ] Intensity: Amplitude.
Chapter 12 Preview Objectives The Production of Sound Waves
Psychoacoustics: Sound Perception Physics of Music, Spring 2014.
Sound – Part 2.
KTH ROYAL INSTITUTE OF TECHNOLOGY Sound, the Auditory System, and Pitch Perception Roberto Bresin DT2350 Human Perception for Information Technology Copyright.
SOUND Longitudinal Wave Travels through some medium Cannot travel through a vacuum How does vibrating drum produce sound? Skin moving up presses air.
Properties of Sound Physical Science Ms. Pollock
Last lesson Learning to listen Sound as vibrations Amplitude and volume Frequency and Pitch Range of human hearing.
Sound in everyday life Pitch: related to frequency. Audible range: about 20 Hz to 20,000 Hz; Ultrasound: above 20,000 Hz; Infrasound: below 20 Hz Loudness:
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.
David Meredith Aalborg University
Sound and Intensity Transverse vs. Longitudinal Waves Sound Frequency
The Physics Of Sound Why do we hear what we hear?
SOUND & THE EAR. Anthony J Greene2 Sound and the Ear 1.Sound Waves A.Frequency: Pitch, Pure Tone. B.Intensity C.Complex Waves and Harmonic Frequencies.
HEARING MUSICAL ACOUSTICS Science of Sound Chapter 5 Further reading: “Physiological Acoustics” Chap. 12 in Springer Handbook of Acoustics, ed. T. Rossing.
SOUND PRESSURE, POWER AND LOUDNESS MUSICAL ACOUSTICS Science of Sound Chapter 6.
24.3 Sound  Sound is a traveling oscillation of atoms or pressure.  When they are pushed by the vibrations, it creates a layer of higher pressure which.
Sound Pressure, Power, and Intensity Chapter 6. Sound Pressure/Power/Intensity All three terms describe physical sensations. All three are perceived on.
Encoding and Simple Manipulation
Intensity of a Spherical Wave
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
Sound “A sound man…”. Frequency The frequency of a sound wave is perceived as the pitch (note) –High frequency → high pitch → high note –“Middle C” has.
Chapter 16: Sound 16-1 Characteristics of Sound 16-3 Intensity of Sound: Decibels 16-4 Sources of Sound: Vibrating Strings and Air Columns.
Session 18 The physics of sound and the manipulation of digital sounds.
Digital Audio I. Acknowledgement Some part of this lecture note has been taken from multimedia course made by Asst.Prof.Dr. William Bares and from Paul.
Chapter 12 Preview Objectives The Production of Sound Waves
SOUND PRESSURE, POWER AND LOUDNESS
Consider the possible standing waves that could exist on a 6.00-m long stretched rope (fixed at both ends). a. What is the wavelength of the fourth harmonic.
Properties Of Sound Sound waves are produced as longitudinal waves by compressions and rarefactions in matter. The medium for sound waves can be solid,
Physics Section 12.2 Apply the sound properties of intensity and resonance Intensity is the rate at which energy flows through a unit area perpendicular.
SOUND FUNDAMENTALS Prepared by:SHUBHAM UMAKANT GUPTA En no
HEARING MUSICAL ACOUSTICS Science of Sound Chapter 5 Further reading: “Physiological Acoustics” Chap. 12 in Springer Handbook of Acoustics, ed. T. Rossing.
Physics Acoustics for Musicians selected slides, March 5, 2002 Loudness at different frequencies Critical band Masking The ear Neurological response.
4. The Ear and the Perception of Sound (Psychoacoustics) Updated May 13,
Chapter 16: Sound 16-5 Quality of Sound, and Noise; Superposition 16-6 Interference of Sound Waves; Beats 16-7 Doppler Effect HW problems: Chapter 16:
Intensity.
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
Peripheral Auditory System
L6 and L7 Sound Intensity, Sound Level/Loudness (Decibels), The Ear
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
EE Audio Signals and Systems
Hearing and Mechanoreceptors
Sound Intensity and Resonance
Psychoacoustics: Sound Perception
Sound Intensity = Power / Area (Watts / Meter2)
Lecture 18 Sound Levels November 1, 2004.
Chapter 16: Sound.
Sound 13.2.
Presentation transcript:

Physics 371 - Acoustics for Musicians selected slides, February 28, 2002 Sound intensity Level The decibel (dB) Sound pressure Examples Sensitivity curves (Phon)

Hearing: loudness Sound Intensity Level I: level I is measured by power/m2 (Watt/m2 = W/m2) range from hearing threshold to pain level : intensity level at threshold of hearing: I 0 =10 -12 W/m2 intensity level at threshold of pain: 1 W/m2 (expressed in sound pressure, threshold is 2x 10-5 N/m2, which is about 1/10,000 of pressure of sheet of paper on table) If we measure intensity of sound in relation to threshold intensity the answer will vary from 1 to 1,000,000,000,000 !! How can an organism accommodate this huge intensity range? How can we better express the intensity level?

Answer: logarithmic response of the ear Ear and brain is made such that equal factors in intensity cause equal increments in loudness. if we call threshold intensity = 1: Intensity I: 1 10 102 103 104 ……..1010 1011 1012 log I : 0 1 2 3 4……….. 10 11 12 10log I: 0 10 20 30 40 ……… 100 110 120 dB this is the DECIBEL SCALE of Sound Intensity Level: Intensity level in dB: (can be used to compare any two intensity levels

What does one dB change in loudness sound like? demo: 1 dB steps 3 dB steps 5 dB steps examples: a) calculate the intensity ratio for a 1 dB step. b) one dynamic step (ppp - pp - p - mf - f - ff - fff) about 6dB find intensity ratio for each step. comments on buying audio equipment: flatness of response, power, freq. rolloff Adding sounds: DO EXAMPLES ON BLACKBOARD example: add 440 Hz tones of 60dB and 70dB

How is sound pressure P (N/m2) related to intensity I (W/m2) ? When sound PRESSURE P doubles, sound INTENSITY I quadrupes: I is proportional to P2 can use relation to calculate relative sound pressure P2/P1 To calculate absolute sound pressure one uses P0 = 2x10-5 N/m2 example: if f (forte) = 70dB, find sound pressure (Answ: 0.06N/m2)

EXAMPLES (similar to homework): example 1: a cellist can change the string amplitude between 0.1mm and 4mm. We can assume that sound pressure is prop. to string amplitude. What is her dynamic range in dB? example 2: if a crescendo from f to ff increases the sound level by 6 dB find the relative sound intensity find the relative sound pressure example 3: calculate the sound pressure for a 70dB tone (forte) (for comparison: normal athmospheric press - 105 N/m2) example 4: calculate the intensity level in dB when you add sounds of 65dB and 70dB.

Sensitivity of ear as a function of frequency loudness level in Phons tones of different frequencies have the same number of phones if they sound equally loud. the comparison tone is a 1000 Hz tone. example: If a 1000 Hz tone has intensity level of 60 db it is said to have 60 phones - any other equally loud pure tone of different frequency also has 60 phones. highest sensitivity of ear for about 2000 - 5000 Hz DEMO: decrease sound press for 100Hz and for 2000Hz tones by same factor (same dB) - 100Hz becomes inaudible Application: HiFi volume control vs loudness control

Equal loudness level curves: LL= 40 phones

Curves of equal-loudness level N/m2 W/m2 intensity press sound level (dB) Curves of equal-loudness level

Good audio amplifier use automatic loudness control N/m2 W/m2 intensity press sound level (dB) Good audio amplifier use automatic loudness control

Neural Response of Ear: the Neural Transmitters anatomy of the ear: Show overhead transparencies (see Fig. 1 p. 88 Backus) Basilar membrane length about 35 mm; 3.5 mm per ocatave 30,000 receptors. Localization of freq. sound is transmitted to the brain not as a wave shape but as individual pulses ("discharge" of nerve cell). Pulses have same height independent of stimulus, average pulse rate depends on loudness level. time distribution of pulses encodes wave shape

Rose et al. J. Neurophysiology time interval between nerve impulses for different frequencies. rate 30 spikes/s at 70 dB rate 120 spikes/s at 70 dB 217 Hz 600 Hz 192 Hz 460 Hz 167 Hz 365 Hz 5 10 15 20 ms 5 10 15 20 ms 5 10 15 20 ms

30dB 70dB 60dB 20dB 5 10 15 20 ms