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  • 8/6/2019 DESIGN OF TRANSPORT NOISE BARRIERS

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    Ecology and Environmental Protection

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    DESIGN OF TRANSPORT NOISE BARRIERS

    Assoc. Prof. Nikolai Nikolov1, D.Sc.

    Prof. Metodi Mazhdrakov2, D.Sc.

    Dobriyan Benov3

    1Institute of Building Physics, Technology and Logistics,Bulgaria

    2University of Mining and Geology St. Ivan Rilski,Bulgaria3ACMO-2006 LTD,Bulgaria

    ABSTRACT

    Transport noise barriers areecologicalstructuresthataredesignedandbuiltalongtheroads

    (motorways, expresswaysandrailwaysetc.), inorder to reducethenoiselevels tothelimitvalues forurbanareasandinrooms of buildings. Assessment of theeffectiveness of

    thebarrieriscarriedouttheoretically, empiricallyorby a combination of bothmethods. Toautomatethedesign of thinnoisebarriersarecreatedfourmodulesfromtheseriesScreen *,

    whicharepart of thesoftwarepackageforacousticcalculationsSoundBG.

    Keywords:noise barriers, acoustical design, software

    1. Definition, acousticefficiency and classification of transport noise barriers

    Transportnoisebarriersareecologicalstructuresthataredesignedandbuiltalongtheroads

    (motorways, expresswaysandrailwaysetc.), inorder to reducethenoiselevels to

    thelimitvalues forurbanareasandinrooms of buildings.The barriers are made of different

    sizes (length and height), of different construction materials, have various cross sections

    and architectural appearance. In acousticspoint of view,the design of transport noise

    barriers cant be standard (uniform), as opposed to elements from which are theydesigned. This complexity lies in their construction-acoustical design, which is a

    function of many requirements, factors, phenomena and parameters. From an economic

    perspective, this factor is leading to determine the value of the facility [1].

    Transport noise barriers can be defined as solid, practically adequately soundproofed

    enclosures,that creates a sound shadow zone behind them by breaking the direct

    distribution of noise in the line of direct sight from the center of the source to the point

    of impact (assessment point), where the noise level decreases due to diffraction of sound

    waves (Fig. 1).

    The effect of the noise barrier is based on acoustic processes taking place after itsconstruction. The main effect of noise reduction is achieved thanks to the creationof

    acoustic shadow due to diffraction of sound on the free edge of the barrier.

    Quantitativemeasure of noise protectionby thebarrierisitsacousticefficiency,

    definedasthedifferencebetweennoiselevelsintheassessmentpointbeforeandafterconstruction of thebrrier, with allthe same other conditions.

    According to thedesignandachievedefficiency, barriersaredividedintoseveralclasses [1].

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    1. Thin barriers. Hei ht ratio is 2 to 6 m, and their acoustic efficiency is bet een 6 and

    18 dB .

    Fi . 1.Acoustic desi n of a thin barrier

    2. Thick barriers.Hei ht ratio is 2 to 3 m, thickness is over 3 m, and their efficiency is

    bet een 5 and 10 dB A).

    3. Acoustic tunnels. Their efficiency is 25-30 dB (A).

    4. Compound barriers - a combination oft o types of barriers. Their hei htis 3 to 5 m,and efficiency bet een 12 and 17 dB(A). The most common combination is

    embankment with a thin barrier.

    In the following statement will be considered acoustical design only ofthin barriers that

    are applied most widely in Europe and the USA.

    2. E i i calculati of thi barri r.

    Efficiency evaluation of the barrier is carried out theoretically, empirically or by a

    combination of both methods. The following formulas solves the so-called "right

    problem", i.e. calculated is efficiency with given height ofthe barrier and its location in

    relation to the noise source and the assessment point (Fig. 1).

    Example oftheoretical and empirical determination of the efficiency of the barrier are

    the works ofMaekawa, who has studied the diffraction in a thin barrierin experimentalconditions [2].

    For an infinite noise source (car stream) from Maekawas studies is obtained, that the

    efficiency ofthe barrieris:

    ( ) , :

    )1(dB( ),,.1.

    2

    .

    2.

    !!(

    P

    HNL

    NB

    whereNis Fresnels number;

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    length of the sound wave, m;

    difference between the shortest distance from the noise source (1) to theassessment point (2) and the road that passes the diffracted sound, m.

    From Fig. 1 is that:

    )2(m.,2212

    21

    2

    2

    2

    2

    2

    1

    2

    1 hhddhhdhhddBA !!H

    Formula (1) hasphysicalmeaningwhen 0"5 , i.e.ifsoundis diffractedthethe upperedge

    of thebarrier. When 0!5 itisassumedthattheefficiency of thebarrier is 5 dB(A).

    Themainfactorsthatdeterminetheefficiency of thebarrier is determined by formulas (1)

    and (2). These are:

    - heightof the barrierh;- lengthofthesoundwave; for car streams is accepted m84.0!P , for railway

    transport - m42.0!P ;

    - geometric parameters of the location of the source (d1,h1) and of the assessmentpoint(

    d2,h

    2);- type of the source with infinite or finite length.Formula (1) refers to thenoisesourcewithinfinitelength; for a singlenoisesourceor a

    sourcewith finitelength (railways) thecorresponding formula is:

    )3(d ( ).,03.159.12

    22.0

    22.0

    !!(

    P

    HNL

    NB

    Whentheassessmentpointislocatedin a room,

    theoverallreductioninnoiselevelinthepresence of thebarrierwillbe:

    )4(dB(A),,CARNBLLLLL ((((!(

    7

    where RL( is the recuction in noise level, because of the increased distance from source,dB(A);

    AL( -reductioninnoiseleveldue to absorption of soundenergyin the air, dB(A);

    CL( - soundinsulationfromairbornenoise of thesurroundingstructure, dB(A).

    For open space dB(A)0!(C

    L .

    For a continuoussource (carstream) the reductioninnoiseleveldue to increasing

    distancefromsource is:

    )5(dB(A),,lglg

    lg

    1100

    rr

    rLR

    !( T

    N

    whereis the average distance between the unit sources in the stream, m;

    r distance from noise source to assessment point, m;

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    r0 basicdistancefordetermination of thenoisecharacteristics of thestrem(for car

    streams m5.70 !r ).

    With a sourcewith finite length, thereductioninthenoise levelbetweenpointsAandB,

    whichlieson normal to themiddle of thesource,at a distancesrAandrB, is

    )6(dB(A).,)(

    )(lg20

    B

    A

    Ad

    rf

    rfL !(

    Ingeneral, thefunctionf(r)issignificantlymorecomplexthanformula (5) [3]. For a smallnumber of individual sources - 2, 3 or 4, the function is simplified [4]. Forexample, for

    foursourcesat a distanceapart, we have:

    (7),111

    )(21

    2

    2

    2

    1rrrr

    rfA

    !

    where .2,1,5.0 222 !! iirr Ai N

    The formula forf(rB)is analogical.

    The reduction in noise level due to absorption of sound waves fromtheairis:

    )8(dB(A).,005.0 rLA

    }(

    Thelength of thesides of thebarriermustnotallowdirectsound, whichispassedthroughit, to

    exceedthenoiselevel (Fig. 2). Taking into account the particularities of power

    summation, we obtain:

    )9(d ( ),,5'' (((u(( ARNBAR LLLLL

    wherethereductions 'RL( and 'AL( dependsonthelength of theside of thebarrier.

    Fig. 2.Determination of thelength of thebarrier

    From Fig. 2 is that the total length of the screen:

    )10(m,,1'

    2

    2

    2N

    !

    r

    rdW

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    where 'r isthedistancefromtheassessmentpoint to thenearestnoise

    sourcethatisoutsidetheactionofthebarrier, m;

    - the length ofthe protected object, m.

    3. Determi i the required efficiency.

    Noiseregimeintheassessmentpointdependsonthenoisecharacteristics of thesourceL0, the

    noise reductionfromthescreen, thedistanceandsurroundingstructures,

    aswellaspermissible noise levelLLD, whichisregulatedbythelegal documents [5].

    Inorderto meetthelegalrequirementsitis necessary

    )11(.d (A),0 CARNBLD LLLLLL ((((e

    Fromformula (10) we definetherequired (design) efficiency ofthebarrier:

    )12(.dB( ),0 LDCARNB LLLLLL (((!(

    Therelationshipbetweendesignheight of thebarrierandrequiredefficiencyisthe"inverseproblem" of theformula (1). Inthiscase, theunknownparameter istheheight ofthebarrierh, whichleads to a transcendentalequation.

    4. Software.

    To automatethedesign of thinnoisebarriersarecreatedfourmodulesintheseriesScreen *,

    whicharepart ofthesoftware packageSoundBG [6].

    The modulesScreen H VarandScreenHLVarintendedfor a feasibilitystudy of thesite.WithScreen H Varcan be finded thedependenciesbetweentheefficiency of thebarrier

    anditsheightanddistance to theassessmentpoint (Fig. 3) and/orheight ofthat point (Fig.

    4).

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    Fig. 3.ModuleScrren H Var, executedwith a

    variabledistancebetweenthebarrierandassessmentpoint;the height oftheassessmentpointis 12.5 m.

    Fig. 4.ModuleScrren H Var, executedwith a variableheight ofthe assessment point; the

    distancebetweenthebarrierandassessmentpointis30 m.

    The moduleScreenHLVarexpandsthepossibilitiesforpreliminaryanalysis.

    Inninegraphsare showthedependenciesbetweentheparameters of thebarrier - efficiency,

    height, length, andnoisecharacteristics of thenoisesource, theindex of

    airbornesoundinsulationfromthesurroundingstructureandregulatorynoiselevel.

    The module Screen Project calculatestherequiredheight of thebarrier

    underspecificconditions: geometry, noise levelsintheprotectedarea, soundproofing of

    thepremises. The calculation is carried outin transverse acoustic profiles (Fig. 5).

    Fig. 5.Computiveacousticprofile[7]

    As a result, for eachprofile aregiventhenecessaryheightandlength ofthebarrier.

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    Fromthecalculatedvalues areobtainedthe finaldesignheights,

    takingintoaccounttwoadditionalrequirements.

    1.1. Sizesof the barrier mustbemultiples of thedimensions oftheelementsthatareassembledorconstructed, eg. panels withsizes0.5x3 m.

    2.Theheight of thebarrier mustberelativelyconstantforlongstretches of theroute.The efficiency of the barrier with the adopted design sizes is assessed with module

    Screen Project B, which performs by the same computing profiles. Depending on theresults, follows different solutions - to increase the design height, increasing the sound

    insulation of the surrounding structure of the upper floors of buildings, etc.

    *

    Thedescribedtechnologywasappliedforthedesign of transport noise

    barriersinthereconstruction of theoverheadroad to BrusselsblvdinSofia [7].

    REFERENCES

    [1] .. . : . , 2006. . 236.

    [2] . . .:

    . : -. 1986. 423 .

    [3] .. ,

    .. ,5, , 2009, . 224-

    228.

    [4] .. . . , No. 1, , 2011.

    [5] 6 , ,

    ,

    , , 58/2006.7.

    [6] Nikolov N.D., Mazhdrakov, M.G., Benov D.M., Trapov G.I. Software

    suiteforacousticalcalculationsSoundBG. 11th International GeoconferenceSGEM 2011,

    Albena, Bulgaria, 2011.

    [7] .., .., .., .. . , . . .

    , , 2011, . 1.