31-10-12 Edu Set Sound Insulation & Acoustics

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    GENERAL INTRODUCTION Sound is generated in the air when a surface is

    vibrated.

    The vibrating surface sets up waves of compressionand rarefaction.

    To understand it let us take example of tuning fork

    2PRESENTATION BY MANISH KUMAR LEC.ARCHITECTURE AT PATIALA

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    GENERAL INTRODUCTIONI have drawn three pictures of a

    tuning fork to help you visualize

    how air molecules might look

    around a tuning fork.

    When the tuning fork is at rest,

    the fork is surrounded by

    molecules in the air.

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    GENERAL INTRODUCTIONAs a tuning fork's prongs move

    apart because of a vibration.

    The molecules ahead of it are

    crowded together.

    They look like they are being

    pushed together. They bump

    each other.

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    GENERAL INTRODUCTIONAs the tuning fork's prongs

    come back together, it leaves a

    region that has fewer

    molecules than usual.The region of a sound wave in

    which the molecules are

    crowded together is a

    compression.

    The region of a sound wave in

    which particles are spread

    apart is a rarefaction.

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    GENERAL INTRODUCTIONAs a tuning fork vibrates, it causes molecules in

    the air to move.

    The molecules bump into other moleculesnearby, causing them to move.

    This process continues from molecule tomolecule.

    The result is a series of compressions andrarefactions that make up sound waves.

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    GENERAL INTRODUCTIONAnd these compression and rarefactions sets the

    ear drum vibrating.

    The movements of ear drum are translated by the

    brain into sound sensation.

    So, we really don't hear with our ears - we hear

    with our brains!

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    GENERAL INTRODUCTIONShape (dish

    type) of theouter ear ishelpful in

    receivingsound waves.

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    GENERAL INTRODUCTIONHere's How It Works Sound vibrations, or sound waves, are collected by

    the OUTER EAR.

    And travel into the ear canal, where they bump upagainst the ear drum.

    The EAR DRUM vibrates in sympathy with these

    sound waves. As it vibrates, it moves a series of tiny bones in

    the MIDDLE EAR

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    GENERAL INTRODUCTION

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    Intensity and loudness of sound Loudness of a sound corresponds to the degree of

    sensation depending upon the intensity of sound and

    sensitivity of ear drums.

    It may also happen that the same listener might give

    different judgments about the loudness of sound of

    the same intensity but of different frequencies as the

    response of the ear is found to vary with the frequency

    of vibration.

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    Frequency and pitch of sound

    Frequency or pitch is defined as the number of cycle

    which a sounding body makes in each unit of time.

    It is measure of the quality of sound. The sensation of pitch depends upon the frequency

    with which the vibrations succeed one another at the

    ear.

    Greater the frequency the higher the pitch.

    And the lesser the frequency the lower the pitch.

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    Frequency and pitch of sound The audio range falls between 20 Hz and 20,000 Hz. This

    range is important because its frequencies can be detected

    by the human ear. A frequency is expressed in terms of Hz(Hertz)

    and it determines pitch of sound source. They can be

    categorized as:

    Low tones sound of urban road traffic.

    Mild tones sound of piano notes.

    High tones sound of single tea kettle.

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    The behavior of sound propagationIt is affected by many things:

    The speed of sound within the medium depends upon

    temperature of the medium ,which in turns effect thedensity and pressure of the medium..

    The propagation is also affected by the motion of the

    medium itself. For example, sound moving through wind is further

    transported towards the direction of wind.

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    The behavior of sound propagation The viscosity of the medium also affects the

    motion of sound waves.

    It determines the rate at which sound is

    attenuated.

    For many media, such as air or water, attenuationdue to viscosity is negligible.

    Sound cannot travel through a vacume.

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    The behavior of sound propagation

    It travels much faster in solids and liquids then inair.

    The velocity of sound in atmospheric air at 20

    degree centigrade is 343 meter per second. The velocity of sound in pure water is 1450 meter

    per second.

    The velocity of sound in bricks is 4300 meter persecond.

    The velocity of sound in concrete is 4000 meterper second.

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    The behavior of sound in enclosures

    When the sound waves strike the surfaceof room three things happen

    (1) Some of the sound is reflected back in the room.

    (2) Some of the sound energy is absorbed by the

    surfaces and listeners of the room/hall .

    (3) And some of the sound is transmitted out of the

    room through vibrations of f loors, walls and

    ceilings.

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    The behavior of sound in enclosures

    The amount of sound reflected and absorbed

    depends upon the different surfaces of room.

    And the sound transmitted outside the room will

    depend upon .

    The sound insulation properties of walls , f loors

    and ceiling etc. .

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    Reflection of sound waves.

    Reflection of sound waves is exactly the same asthat of light waves.

    That is angle of incidence is equal to the angle ofreflection. *c

    *c *c

    INCIDENT WAVEREFLECTED WAVE

    REFLECTING SURFACE.

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    Reflection of sound waves.

    The reflectedwave

    frontfrom a flat

    surface are alsospherical and their

    centre of curvature

    is the image of

    source of sound.

    FLAT REFLECTORWAVE FRONT

    SOUND

    SOURCE

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    Reflection of sound waves.Sound waves reflected ata convex surface aremagnified and areconsidered bigger.

    They are attenuated andtherefore weaker.

    So convex surface may beused with advantage tospread the sound wavesthroughout the room.

    WAVE FRONT CONVEXREFLECTOR

    SOUNDSOURCE

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    Reflection of sound waves.

    The sound waves reflected ata concave surface areconsidered smaller.

    The waves are most condensedand therefore amplified.

    The concave surface may beprovided for concentration ofreflected waves at certainpoints.

    WAVE FRONT

    CONCAVE REFLECTOR

    SOUNDSOURCE

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    Acoustics general introduction The scientific study of the phenomenon of

    sound is known as Acoustics.

    Acoustics as applied to buildings is the scienceof sound which assures the optimumconditions for

    Producing sound/speech/music

    Listening of sound/speech/music

    Recording /editing of sound etc.

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    Acoustical Interaction

    Acoustics means to work on these threeparameters and improve sound experience.

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    Acoustical Interaction

    Sound is attenuated by absorption Historically, the primary focus of acoustics was

    the use of absorbing surfaces to control thereverberation times and loudness of spaces.

    Redirected by reflection

    Uniformly scattered by diffusion Good architectural acoustic design requires an

    appropriate combination of absorptive,reflective and diffusive surfaces

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    Acoustics general introduction

    For better acoustical results the construction andapplication of sound absorbents and soundreflective materials should be carefully selected

    and placed.

    This will help in providing better quality of audiovideo sensations to viewers/ listeners.

    Proper acoustical planning can reduce orcompletely eliminate defects related to sound,which are called acoustical defects.

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    Acoustical defects

    List of acoustical defects

    Reverberation.

    Formations of echoes.

    Sound foci.

    Dead spots.

    Insufficient loudness.

    Exterior noises.

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    Acoustical defects (Reverberation)

    Reverberation is the persistence of soundin the enclosed space , after the source of

    sound has stopped. Reverberant sound is the reflected sound

    , as a result of improper absorption.

    Reverberation may results in confusionwith the sound created next.

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    Acoustical defects (Reverberation)

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    Acoustical defects (Reverberation)

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    Reverberation time & quality of sound

    Reverberation time should remain within limits as perIndian Standard Code: 2526-1963.

    Sr.No.

    RECOMMENDED TIME INSECONDS

    ACOUSTICS

    1 0.50 to 1.50 Excellent

    2 1.50 to 2.00 Good

    3 2.00 to 3.00 Fairly good

    4 3.00 to 5.00 Bad

    5 Above 5.0 seconds Very bad

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    Formation of echoes. Echo's

    Not all sound that hits matter is absorbed. Someof it is reflected. That means sound bounces offthe solid matter the way a tennis ball bounces offa wall. Sound reflected back to its source is anecho.

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    Formation of echoes.

    An echo is produced when the reflected sound wavereaches the ear just when the original sound from thesame source has been already heard.

    Thus there is repetition of sound.

    The sensation of sound persists for 1/10thof a secondafter the source has ceased.

    Thus an echo must reach after 1/10th

    second of thedirect sound

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    Formation of echoes. Multiple echoes may be heard when a sound is

    reflected from a number of reflecting surfaces

    placed suitably.

    This defect can be removed by selecting proper

    shape of the hall .

    And by providing rough and porous interior

    surfaces to disperse the energy of echoes.

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    Dead spots.

    This defect is the out come of formation of soundfoci.

    Because of high concentration of reflected soundat sound foci , there is deficiency of related sound

    at some other points. These spots are known as dead spots where sound

    intensity is so low that it is insufficient forhearing.

    This defect can be removed by suitably placingdiffusers and reflectors.

    Right proportions of internal spaces.

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    Dead spots.

    Geometrical shape of roof helps in proper distribution of sound

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    External noise External noises from vehicles , traffic engines ,

    factories , machines etc. may enter the hall either

    through the openings or even through walls and otherstructural elements having improper sound

    insulation.

    This defect can be removed by proper planning of thehall with respect to its surroundings and by proper

    sound insulation of external walls.

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    Acoustical design of halls The initial sound from the source should be of

    adequate intensity so that it can be heard

    throughout the hall .

    For halls of big sizes suitable sound amplification

    system should be installed.

    The sound produced should be evenly distributed

    so that there is no dead spots and sound foci.

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    Acoustical design of halls The boundary surface should be so designed that

    there are no echoes or near echoes.

    Desired reverberation time should be achieved by

    proper placement of absorbents on wall.

    The out side noise should be eliminated.

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    Physical Design Principles for halls

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    Physical Design Principles for halls

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    Physical Design Principles for halls

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    Physical Design Principles for halls

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    Physical Design Principles for halls

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    Physical Design Principles for halls

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    Physical Design Principles for halls

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    Acoustics materials

    Carpet is an outstanding sound

    absorptive material. When

    properly selected, carpet absorbs

    airborne noise as efficiently as

    many specialized acoustical

    materials. No other acoustical

    material performs the dual role of a

    floor covering and a versatile

    acoustical aid.

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    Acoustics materials

    QUIET BARRIER HDA flexible, 2lb per sq./ft. 1/4in. thick, high density

    material with a smoothsurface designed to reducenoise transmission betweentwo spaces. Applicationsinclude reducing airborne

    noise transmission throughwalls, ceilings and floors

    54PRESENTATION BY MANISH KUMAR LEC.ARCHITECTURE AT PATIALA

    http://www.soundprooffoam.com/quiet-barrier.html
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    Acoustics materialsQUIET BARRIER MD

    A flexible, 1lb per sq./ft. 1/8 in.

    thick, high density material

    with a smooth surface

    specially engineered to

    reduce noise transmission

    between two spaces.

    55PRESENTATION BY MANISH KUMAR LEC.ARCHITECTURE AT PATIALA

    http://www.soundprooffoam.com/econo-barrier.html
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    Acoustics materialsTough core Ceiling Tiles

    High-performance composite

    ceiling panel. Especially well-

    suited to minimize sound

    transmission between adjacent

    spaces sharing a common attic

    space. Available in a variety of

    finish options and edge details.

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    http://www.soundprooffoam.com/tufcore-ceiling-tiles.html
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    Acoustics materials

    Isotrax

    Complete soundproofing

    system for walls and

    ceilings. Blocks andisolates sound, reduces

    noise from traveling

    through building materials.

    New or existingconstruction.

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    http://www.soundprooffoam.com/isotrax.html
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    Acoustics materials

    damping tiles used for noise absorption.

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    Sound insulation general introduction

    Unwanted sound reaching the ears is called

    NOISE.

    It may be due to frequency of sound.

    It may be due to intensity of sound .

    Or it may be due to the combination of both

    frequency and intensity of sound.

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    PRESENTATION BY MANISH KUMAR LEC.ARCHITECTURE AT PATIALA 61

    Sound insulation

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    Sound insulation general introduction

    So sound insulation is the measure by whichtransmission of sound / noise from inside to out side(vice versa ) or from one room to other is prevented.

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    Sound insulation ( effects of noise) It creates discomfort.

    It has adverse effect on blood pressure , sleep andcauses muscular strains.

    It leads to fatigue and decreases the efficiency of aperson.

    It takes away essence of music and speech.

    It disturbs concentration.

    Prolonged exposure to noise may result in temporarydeafness or even nervous breakdown.

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    Classification of noise.From the origin point of view noise may be of two

    types:-

    Out door noise.

    Indoor noise.

    And noise may also be classified as

    Air borne noise or sound

    Structure borne noises or impact noises or sounds.

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    Sources of out door noises.

    OUT DOOR NOISES ARE CAUSED BY:-

    Road traffic.

    Railways.

    Climatic conditions.

    Aero planes.

    Moving machines.

    Machines in nearby factories or buildings etc.

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    Transmission loss (TM) of sound

    When sound is transmitted from source ororigin to the adjoining room/ area, reductionin sound intensity takes place.This is known as transmission loss (TM)Measured in decibels (dB)

    60 decibels 40 decibels

    TM=60-40=20 DECIBELS.

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    Types of sound insulating materials

    Non porous rigid.

    Porous rigid materials.

    Non rigid porous flexible materials.

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    Types of sound insulating materials Non porous rigid

    Brick masonry plastered on both sides

    Stone masonry structures

    Concrete structures RCC Structures

    Porous rigid materials.

    Light weight concrete

    Cellular concrete

    Gypsum board partitions

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    Types of sound insulating materials

    Non rigid porous flexible materials

    Perforated boards

    Compressed fiber boards

    Pulp boards

    Mineral wool boards

    Acoustic tiles /sheets

    Glass wool

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    Types of sound insulating materials

    Non rigid porous flexible materials

    Cobalt quilt

    Wood wool boards

    Curtains

    Foams

    Celotex boards

    Cane fiber etc.

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    Sound insulating techniquesThere are some construction techniques also which

    are adopted for sound insulation.

    Double wall construction.

    Cavity wall construction. False ceiling.

    Hollow block construction.

    Double pane windows. Baffle blocks, honey combs etc.

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    Sound insulating techniques Double wall construction .

    BOARDS WOODENSTUDS

    SOUND ABSORBING BLANKETBOARDS

    WOODEN STUDS

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    Sound insulating techniques False ceiling.

    REINFORCED CONCRETE ROOF

    SUSPENDERS

    FALSE CEILING

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    Sound insulating techniques Hollow block construction.

    COMPRESSED CONCRETE HOLLOW BLOCKS

    HOLLOW

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    Thank you and enjoy sound