Sub-bottom Profiler ORE Model 1036

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    OPERATING ND

    MAINTENANCE MANUAL

    FOR THE

    O.R.E.MODEL 1036

    HIGH

    POWER

    MULTI-FREQUENCY

    S U ~ O T T O M PROFILING SYSTEM

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    OPERATING AND MAINTENANCE MANUAL

    FOR THE

    O.R.E. MODEL 1036

    HIGH POWER MULTI FREQUENCY

    SUB-BOTTOM

    PROFILING

    SYSTEM

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    CONTENTS

    Page

    l INTRODUCTION

    1-1

    2. GENER L

    DESCRIPTION

    2-1

    2.1 Major

    Sub-Systems

    2-1

    2 2

    Transceiver

    2-1

    2 2 1 Receiver

    2-1

    2. 3 Prec i s ion

    Recorder

    2-2

    2 4

    Towed Transducer Vehicle

    Sub-System

    2-4

    2 4 1

    General

    2-4

    2 4 2

    Fish

    2-4

    2 4 3

    Towing Pos i t ion

    2-4

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    4.

    3.3

    Tow

    Cable-Model

    143A

    3.4 Winch

    3.5 In te rconnec t ing Cable

    (Winch

    to

    Transce iver

    INST LL TION ND OPER TION

    4.1 Operat ing

    Notes

    4 .1 .1 Towing

    4 .1 .2

    Transmit ter

    Power

    4 .1 .3 Transmit ter

    Frequency

    4 .1 .4 Pulse Dura t ion

    4 .1 .5 Receiver Bandwidth

    4 .1 .6 Adjustment

    fo r

    Optimum Resul ts

    3-5

    3-5

    3-5

    4-1

    4-1

    4-1

    4-2

    4-2

    4-2

    4-3

    4-3

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    Page

    5 2

    Propagat ion

    Loss

    5 2

    5 2 1

    Spreading

    Loss

    5 2

    5 2 2 Absorpt ion

    5 2

    5 3

    Ref lec t ion

    and

    Refrac t ion

    5 3

    5 3 1 Ref rac t ion

    5 3

    5 3 2

    Ref lec t ion

    5 3

    5 4

    Sca t te r ing

    and

    Reverbera t ion

    5 4

    5 4 1 Volume

    Reverbera t ion

    5 4

    5 4 2 Surface

    Reverbera t ion

    5 4

    5 5

    Noise

    5 5

    5 5 1 Background

    Noise

    5 5

    5 5 2

    Reverbera t ion Noise

    5 7

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    LIST

    OF FIGUR S ND

    DR WINGS

    Figure 2 1

    Figure

    2 2

    Figure

    4 1

    Figure

    4 2

    Figure

    4 3

    Figure

    4 4

    Figure

    4 5

    Figure

    4 6

    Figure

    4 7

    Figure

    5 1

    O.R.E. Model 1036 Sub Bottom Pr o f i l i ng

    System

    O.R.E. Sub Bottom Prof i l ing System

    O.R.E. Model

    T610

    Junc t ion

    Box

    North Sea

    Fine

    Sand

    Bottom

    North Sea Sand Bottom

    Decca N V Survey

    Decca Survey

    Decca Survey

    Pipe l ine

    Locat ion

    A1200 0001

    Miss i s s ipp i River Gulf Out le t Channel

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    1.

    INTRODU TION

    The

    O.R.E.

    Model 1036 Sub-Bottom Prof i l i ng System i s

    designed to obta in accura te ,

    continuous

    acous t ic pro f i l e s of

    l aye r s

    beneath

    the sur face of the sea bottom as wel l as pre -

    c i s i on bathymetr ic

    data .

    Records

    are obta ined by t ransmi t t ing high-power pulses

    of

    acous t ic

    energy from a

    t ransducer

    array towed in a fa i red

    vehic le , or

    f i sh ,

    by the survey

    vesse l .

    Because of

    the c lean

    hydrodynamic

    c h a ra c t e r i s t i c s

    of

    the f i sh ,

    opera t ion of

    the

    system

    can

    be

    mainta ined

    a t normal

    c ru i s i ng

    speeds and

    rough

    sea condi t ions

    without de l e t e r i ous e f fec t s on the acous t ic

    t ransmiss ion

    path .

    a

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    opera t ing

    frequency

    pulse

    width

    power

    and

    r ece i ve r

    charac-

    t e r i s t i c s over

    wide

    range.

    Spec ia l ly designed t ransducers

    and rece ive r c i r c u i t r y fu r t he r

    enhance

    the ab i l i t y to reso lve

    echoes from sub-bot tom l ayers

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    2. GENER L DESCRIPTION

    2.1

    Major Sub-Systems

    The Model 1036 Sub-Bottom P ro f i l e r System cons i s t s of th ree

    major sub-systems, connected

    as

    shown

    in

    Figures

    2.1

    and

    2.2.

    1) O.R.E. Model 140, 10 kw Transceiver

    2)

    Prec is ion Recorder

    3) O.R.E. Model

    136 Towed Transducer Vehicle

    and Cable

    Assembly

    2.2 Transceiver

    The Model

    140

    Transceiver conta ins a t r ansmi t t e r whose

    e l e c t r i c a l power

    output

    i s

    cont inuous ly

    var i ab l e from to

    10

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    switch routes

    these

    s i gna l s t o the rece iver , which i s the

    other major component

    of

    the t ransce iver .

    The rece iver i s

    a

    tuned

    ampl i f ie r

    with var i ab l e

    cente r

    f requency, bandpass, and a

    t ime

    varying gain TVG)

    cont ro l .

    Front

    panel

    adjustments permit the center f requency of the

    r ece ive r

    to be adjus ted to

    match

    the t ransmit f requency.

    The

    width

    of the

    bandpass

    f i l t e r can a lso be adjus ted to

    accommo

    da te the spectrum of the t ransmi t t ed pulse and echo).

    The

    TV

    automat ica l ly

    holds

    the

    gain of

    the

    r ece i ve r

    to

    a

    low

    va lue u n t i l

    the

    point in t ime

    where

    the bottom echo

    i s

    received.

    Afte r t h i s in s tan t , the

    gain inc reases l i n e a r ly with

    t ime

    to

    compensate

    for

    the

    a t t enua t ion of

    sound

    through the

    sub-bot tom

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    t r i c a l

    s igna ls from the rece iver , represent ing echoes cause

    curren t to

    pass from the s ty lus

    through the

    paper

    to

    kni fe

    edge extending the width of the paper . The

    paper

    i s

    darkened

    a t t h i s poin t in

    propor t ion to

    the i n t ens i ty of the

    s igna l .

    Since the

    s ty lus

    t r ave l s across the paper a t con-

    s t an t , accura te ly known ra te , the elapsed t ime

    between outgoing

    pulse

    and echo a r r i v a l

    m y now be determined.

    Using an

    assumed

    speed

    of sound in water of

    4 800

    fee t per

    second the

    recorde r

    i s

    ca l ib ra ted

    in uni t s

    of t ime

    or dis tance ,

    e i the r

    fathoms

    or

    meters . Se lec tab le s ty lus sweep speeds represent ing f u l l

    sca l e from 20 to 2 000

    fathoms

    are se l ec t ed by panel

    con

    t r o l .

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    2.4

    Towed

    Transducer Vehicle Sub-System

    2.4 .1

    General

    This sUb-system cons i s t s of the towed t ransducer vehic le ,

    o r

    f i sh ,

    which

    houses

    the

    acous t ic

    t ransducer

    array,

    f a i r ed tow cable , r e t en t i on

    fo r

    connect ing the cable to

    the

    f i sh , deck

    mounted

    winch

    and an in te rconnec t ing cable to

    t i e the

    winch

    end

    of the

    tow

    cable

    to

    the

    t r ansce i ve r .

    2 .4 .2

    Fish

    The f i sh

    cons i s t s

    of hydrodynamical ly fa i red housing

    to enc lose the t ransducer a r ray , means for mounting the array

    in the

    housing

    and s t a b i l i z i n g

    t a i l .

    The

    f a i r ed

    housing

    f loods wi th water

    and

    the bot tom ha l f i s acous t i ca l l y t r ans -

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    2 .4 .4

    Transducers

    The t ransducers accept power from the t r ansmi t te r over

    the range 3.0 to 7.0 kHz. Sound i s

    pro jec ted

    downwards in

    a roughly conical beam 55 degrees wide a t 3.5 kHz

    40

    degrees

    a t 5 .0

    kHz

    and

    30

    degrees a t

    7.0 kHz.

    Maximum permiss ib le

    power

    i n to

    the t ransducers

    i s

    10 kw a t

    a 1

    duty cycle .

    2.5

    Tow

    Cable

    The

    tow

    cable

    combines

    a

    core

    of

    e l e c t r i c a l conductors

    fo r

    the t r ansducer connect ions wi th two l ayers of s t a i n l e s s

    s t e e l oute r armor for t e n s i l e s t reng th . spec ia l re ten t ion

    f i t t i n g

    combining

    a water t igh t e l e c t r i c a l connec t ion

    and

    a

    mechanica l s t reng th connect ion

    i s

    used to connect the

    cable

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      10 KW 7 R A N S M I T P I L S E

    R E C E I VE ferl S G N f tL

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    3. SPECIFICATIONS

    The

    fo l lowing a re genera l spec i f i ca t ions or opera t iona l

    spec i f i c a t i on s

    fo r

    the components which make up

    the

    1036

    System

    3.1

    Model

    140

    Transce iver

    3 .1 .1 Transmi t t e r Sect ion

    Power

    ou tpu t

    Output impedance

    Frequency

    Output

    power adjus tment

    10

    kw RMS

    dur ing key pu l se .

    5, 10, 20, 30, 40, 45, 50, 55,

    60, 75, and

    100

    ohms.

    Cont inuously adjus tab le

    1

    12

    kHz.

    o ther

    f requenc ies ava i l ab l e .

    Cont inuously adjus tab le

    from

    kw

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    3 .1 .2

    Receiver

    Sec t ion

    Input

    impedance

    Frequency

    Bandpass f i l t e r

    Output impedance

    Maximum ou tpu t vol t age

    Sen s i t i v i t y

    10 K ohms

    Adjus tab le 1-12 kHz. Other f r e

    quencies ava i l ab l e .

    Center f requency cont inuously

    va r i ab le

    1-12

    kHz. Bandwidth

    ad jus t ab le

    from 0 .5 kHz

    up

    to

    e s sen t i a l l y f l a t .

    Less

    t han

    100

    ohms.

    4 V

    P-P

    minimum.

    3 microvol t s R S input

    ( fo r

    2

    db s igna l - t o -no i se r a t i o ) produce

    V

    RMS

    output .

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    3 .1 .4

    Specia l Fea tures

    (1) Transmit ter

    and r ece iver f requencies independently ad ju s t

    able .

    (2) Receiver f requency i s matched to

    t r an sm i t t e r

    frequency by

    depress ing

    Receiver Test

    switch and t un ing fo r maximum

    i nd ica t ion on

    VU

    meter.

    The Receiver Tes t

    switch pro-

    duces

    a c a l i b r a t e d s igna l

    a t

    r ece ive r

    input , thus ,

    a l so

    checking

    rece iver

    sens i t i v i t y

    and

    bandwidth.

    (3) VU meter

    i s

    usefu l

    by

    i t s e l f

    for

    l i s t en ing

    to

    remote

    sound sources ( i . e .

    pingers ,

    e t c . ) .

    Transmit ter

    can

    then

    be s e t to

    rece ive

    frequency by

    procedure

    s imi la r

    to

    (2)

    above.

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    Chass is

    Power

    suppl ies

    Size

    Weight

    3.2

    Model 136A

    Spec i f i ca t ions

    3 .2 .1

    Transducer

    Array

    Transducers

    four )

    Frequency

    range

    Bench/rack

    chass i s

    fu l ly enclosed

    and fan cooled.

    Regulated,

    shor t - c i r cu i t proof

    suppl ies used throughout.

    17 inches

    wide

    by 17 inches deep

    by

    7

    inches h igh - - s tandard rack

    or bench

    mounting.

    50

    pounds.

    Model 137D

    3 .0 -7 .0

    kHz

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    Transducer vehic le

    number

    l e s s

    t r ansducer s )

    Upper she l l number

    Lower she l l number

    3.3

    Tow Cable-Model 43A

    Standard l eng th

    Length of f a i r ed

    s ec t i on

    Diameter

    Armor

    Conductors

    D135-3732

    D135-3769

    D135-3770

    100

    f ee t

    30

    f ee t

    3/8 inch

    Two

    l aye r s

    con t r ahe l i c a l l y wound

    s t a i n l e s s s t e e l

    4,

    Number

    19, s t randed copper , po ly -

    propylene

    i n su la t ed ;

    7.7 ohm/1,000 f t .

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    4.

    INST LL TION ND OPER TION

    sepa ra te manual

    for each

    of

    the

    t h r e e

    major

    components

    of the

    system - -

    Model 140 Transceiver

    Pre c i s ion

    Recorder

    and Model 136

    Towed Transducer Vehicle

    System - - exp la ins

    in

    de t a i l

    opera t ion

    maintenance

    deployment and i n s t a l l a t i o n .

    The fo l lowing i s a

    b r i e f

    summary of system

    opera t ion .

    t i o n

    4 .2

    provides s t e p -by- s t e p opera t ing

    procedures .

    4 .1 Operat ing

    Notes

    4 .1 .1 Towing

    Sec-

    The

    f i sh tows wel l a t

    speeds in

    excess o f 12 knots.

    Enough

    cab le should be pa id out

    so

    tha t the f i sh

    swims

    seve ra l f ee t

    below the l eve l o f the

    keel . s u f f i c i e n t

    l eng th of

    f a i r i ng

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    4 .1 .2 Transmi t ter

    Power

    In

    most cases , maximum power 10 kw

    wi l l

    give bes t r esu l t s .

    In very sha l low water a shor t

    i n t e rva l

    of r ing ing a f t e r

    t e rminat ion of the t ransmi t pulse may

    obscure the

    bottom.

    This i s minimized by opera t ion

    a t

    5 kHz.

    n

    i n t e rna l swi tch

    in the t ransce iver (descr ibed in the Transceiver

    Manual) al lows

    the choice of a

    mode

    of opera t ion whereby two of the t r ansduce rs

    in the array are

    used

    exc lus ive ly for t r ansmi t t i ng and t he o the r

    two

    for

    rece iv ing

    only.

    This

    conf igura t ion

    i s

    use fu l

    where

    a wider

    beam

    width i s des i rab le , such as in pipe

    f inding

    app l i -

    ca t ions .

    Cavi ta t ion when the t ransducer

    i s

    l e s s than f i f t e en fee t

    deep

    may reduce power output somewhat;

    however, t h i s does not

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    4 .1 .5 Receiver Bandwidth

    Bandwidth should be as wide as poss ib le and st ll r esu l t

    in an acceptable s igna l - to -no ise

    r a t i o .

    This

    adjustment

    w i l l

    give maximum pulse r i s e t ime and reso lu t ion

    for

    a given pulse

    durat ion.

    4 .1 .6

    Adjustment

    for

    Optimum Resul t s

    As

    noted in

    the

    preceding sec t ion t ransmi t frequency,

    pulse

    dura t ion

    and rece iver bandwidth

    are i n t e r r e l a t e d .

    Optimum

    adjustment

    depends on the r e s u l t s des i r ed

    and

    the

    geology of

    the

    area being surveyed. I t

    i s bes t

    determined by

    experiment .

    4 .1 .7 Time Varying Gain

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    4.1 .8 Recorder

    Scale

    For

    a l l informat ion

    concerning the

    s e t -up

    and use of the

    recorder ,

    r e f e r

    to the

    spec i f i c

    Recorder Manual.

    4.2

    Opera t ing Procedures

    4 .2 .1 Equipment Required

    I t i s advisable

    to

    have the fo l lowing

    t e s t

    equipment

    ava i l ab l e to ope ra t ing

    personnel fo r

    systems check-out

    and

    t roubleshoot ing:

    a. Simpson 260 VOM or equivalent .

    b. Osci l loscope minimum bandwidth 1 MHZ minimum

    s ens i t i v i t y .05 vjd iv . dual t r a ce .

    c. 100 ohm,

    100

    watt dummy load

    for t r ansce ive r .

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    should wet t ransducer

    faces

    when

    washing i s

    complete.

    DO

    NOT GET

    SILICONE OIL

    OR GREASE

    ON TRANS

    DUCER FACES.

    4 .2 .3

    Operat ion

    a. Visual ly

    inspec t

    recorder s ty lus pa r t s

    for

    any

    poss ib le

    shipping

    damage.

    b. Set recorder

    con t ro l s

    as sugges ted

    in

    t he recorder

    manual.

    c. I n s t a l l r o l l of

    paper -

    plug in recorder .

    d. Turn

    recorder

    ON.

    e. I f necessary , place

    STOP/START

    to

    START

    to

    s t a r t

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    j . Set XMT FREQ

    a t des i red

    operat ing f requency, 3.5

    or

    5.0

    kHz.

    k. Set

    RCVR

    W cont ro l two

    pos i t ions

    from

    CCW.

    This

    corresponds to a

    W

    of

    approximately

    2 kHz.

    Inh ib i t

    keying

    from

    the r ecorder .

    1. Depress

    RCVR TEST

    but ton;

    ad jus t

    RCVR

    FREQ

    fo r

    maxi-

    mum ind ica t ion

    on

    meter .

    Readjustment of RCVR gain

    vern ie r

    may be necessary to keep

    reading

    on

    the

    meter

    sca le .

    m. Restore edge

    keying from the recorder .

    n. Remove

    t r ansce iver top

    cover .

    Check

    to see

    t ha t

    LOAD

    MATCH i s

    in the cor rec t s e t t i ng and t ha t the toggle

    switches are in

    the

    combined pos i t ion .

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    q. STOP

    SHIP.

    Deploy f i sh . Check towing

    cha rac t e r i s

    t i c s as sh ip comes

    up

    to speed.

    NOTE

    I t

    i s advantageous to

    disconnec t f i sh

    cable connector a t winch

    while

    deploying

    and

    recover ing f i sh

    to avoid undue

    twis t ing

    of cable .

    Be

    su re power

    to

    t r ansce i ve r

    i s

    of f

    before d isconnect ing or reconnect ing

    cable .

    r . Turn

    system back on.

    Increase XMT kw to fu l l power

    as before wai t 30

    seconds

    before

    advancing

    power) .

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    w. To

    use

    automatic TVG, se t -up as

    in

    S-T

    above.

    Then

    depress TVG FINDER and se t bl ip a t approximate ly

    one-hal f

    the

    depth,

    but

    be

    sure

    t i s occur r ing in a

    white

    non-noisy)

    sec t ion

    of the water column above

    the

    bottom.

    Rota te TVG THRESH f u l l clockwise and gradua l ly

    ro t a t e

    counter -c lockwise

    un t i l TVG ac t ion resumes.

    Exper i -

    ment

    with the

    s e t t i ng

    of

    the TVG THRESH con t ro l .

    I f

    t i s se t too

    low

    (coun te r -c lockwise ) ,

    the

    TVG c i r

    cu i t i s not

    ac t i va t ed and

    sub-bot tom records a re not

    enhanced. I f t i s se t too high (c lockwise) , the

    TVG

    wi l l

    f i r e

    too

    soon

    on noise) and wil l cause sa tu ra

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    [) CONNECTOR

    /

    RMK

    5

    MP FS

    \ E.NVIROCON

    I

    ,

    ____

    I SMALL

    PIN(TYP)

    o LARGE PIN TYP)

    --l -

    T80

    l

      0+-

    PORT

    __ = :J

    - t - ~ - + - - - + _ T

    (ONN ORE MODEL

    137 A

    TRANSDUCERS

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    4.2 .4

    Recommended Order of

    Shutdown

    Transceiver

    1) Reduce XMIT, W to OFF.

    2) Wait un t i l H.V. i nd i ca to r goes out .

    3)

    Turn POWER OFF.

    Recorder

    1)

    Turn of f Scan

    switch , i f

    appl icable .

    2) Turn

    of f

    Power switch .

    3) Remove remainder of

    paper from recorder .

    Transducer Vehicle

    1) Stop sh ip .

    2) Recover vehic le .

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    shape

    used for sub-bottom pro f i l ing to a more

    forward

    and

    a f t e r

    looking fan

    shape

    pa t t e rn

    idea l

    fo r

    objec t

    loca t ion .

    4.3 .1 Fine

    Adjustments

    As

    in

    sub-bot tom

    pro f i l i ng ac t ua l

    adjus tments of

    the

    t r ansce ive r cont ro l s wi l l depend a grea t deal upon the spec i f i c

    condi t ions experienced.

    The most

    c r i t i c a l

    adjustment wi l l probably be the

    t r ans

    mi t t e r

    f requencies . In genera l t r ansmi t f requencies employed

    in p ipe l ine work are higher than those used

    fo r

    sub-bot tom pro

    f i l i ng . I t i s advisable to s t a r t a t kHz and

    work up.

    Higher f requencies wi l l make smal l e r p ipes v i s ib l e and improve

    r e so lu t ion . Higher f requenc ies however a lso decrease

    penet ra -

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    NOR H

    SEA

    FALL 1976

    FINE SAND BOTTOM

    r

    13 L_1

    ''3&

    :

    .1S

    i e JL .

    ·

    ._.,

    F REQ:5 KHZ SUB BOTTOM

    36 INCH DIAMETER PIPE

    AT BOTTOM OF TRENCH

    .

    \

    ... :; ~ - . : ~ ~

    ., I'

    1.......,.

    - - - '7

    -

    FREQ;

    HZ SUB-BOTTOM

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    \'

    \ ~ ~

    ~ ~

    I.J_

    f\

    ~ - - ~

    ~

    'I ' 'iI

    ,-

    . I

    i

    'f

     

  • 8/16/2019 Sub-bottom Profiler ORE Model 1036

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    1

    - --1

    _ c

    ~ ~ = l : , - i - : : C : ~

    I

    , ' ~ < - ~ ~ .

    ~ ~

    .

    ~ . ~ . -  

    ~ ~ . i - . : '...-0 < . ~ ;

    1

    ·· ·· ..·

    ~

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    I )

    I

    < t

    W

    ::

    J

    9

  • 8/16/2019 Sub-bottom Profiler ORE Model 1036

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    ...

    -  

    --.

    .. . .. I I j

    :: , - ' : ' ~ ~ ' - . r

    ..

    -

    < C

    I

    c;;t

    W

    :::

    >

    (. )

    LL

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    I

    1-'

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    5. THEORY OF SOUN

    Propagat ion of sound in

    sea

    water and the mate r i a l s beneath

    the

    sea

    bed

    i s governed

    by complex se t of phenomena. For

    comprehensive t rea tment

    of

    the theory

    of underwater

    sound

    the reade r

    i s

    r e f e r r ed

    to

    the

    extens ive

    l i t e r a t u r e

    on

    the

    sub-

    j ec t .

    The

    purpose

    of

    t h i s

    sec t ion

    i s to presen t

    to

    the

    user

    unfami l i a r

    with acous t ic

    techniques br i e f qua l i t a t i ve summary

    of the

    fac to rs in f luenc ing

    echo sounding and

    the

    de tec t ion of

    sub-bot tom

    s t r a t a .

    5 .1 Speed of Sound

    The speed of sound in l i qu id

    or

    so l id medium i s func

    t i on

    of

    the proper t i es of the medium. In water the speed

    i s

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    Likewise

    the ac tua l depth of

    sub-bot tom

    l aye r s observed

    with the

    system whi le

    of ten

    expressed

    in

    fathoms or

    fee t

    as

    i nd ica ted

    on the

    recorder sca le wi l l

    in

    genera l be deeper

    than

    ind ica ted .

    The

    depth

    can

    only be determined from sound

    speed measurements made from an

    ac tua l

    core taken

    a t the

    s i t e .

    5 .2

    Propagat ion Loss

    The

    i n t ens i ty

    of sound

    in any

    medium decreases

    with

    d i s -

    t ance

    from

    the source . The

    t o t a l

    decrease a t

    given dis tance

    i s ca l l ed

    the propagat ion loss . This

    loss

    i s

    in

    genera l

    composed

    of

    two

    e lements :

    spreading

    loss

    and

    absorp t ion .

    5 .2 .1 Spreading Loss

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    At

    the

    f requencies 3 .5-7 .0 kHz)

    used with

    the

    Sub-Bottom

    Prof i l e r ,

    the absorpt ion

    l o s s

    in the

    water

    pa th i s smal l

    and

    in fac t

    i s neg l ig ib le for the shal low

    depths

    where the equip

    ment

    i s normal ly

    used.

    5 .3 Ref lec t ion and Refract ion

    The

    laws

    governing

    r e f l e c t i on and r e f r ac t i on of sound in

    l i qu i d and s o l i d media are

    analogous

    to

    those

    governing l i gh t .

    The methods of opt ics ,

    in par t i cu l a r , ray t rac ing , a re

    exten

    s ive ly

    used in ana lys is .

    5 .3 .1

    Ref rac t ion

    In echo sounding and sub-bot tom prof i l ing work, the angle

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    medium. r e f l e c t i ng sur face i s charac te r ized by

    a

    parameter

    known as

    the

    r e f l e c t i on l o s s which i s

    the

    r a t i o

    of

    the in ten

    s i t y of

    the

    r e f l ec ted wave to the i n t ens i ty of the

    inc iden t

    wave a t the sur face .

    5.4

    Sca t t e r ing and

    Reverbera t ion

    f rac t ion

    of the

    energy from

    a sound

    source

    may

    a lso

    be

    re tu rned by

    the process

    of sca t t e r ing .

    Sca t t e r ing r e s u l t s

    from

    p a r t i c l e s

    or

    smal l - sca le inhomogenei t ies

    in

    the medium,

    whose dimensions are

    of the

    order

    of l e s s than a wavelength.

    Sound impinging on these s c a t t e r e r s i s

    r e - r ad i a t ed

    in

    a l l

    di rec t ions . The

    por t ion

    of

    energy r ad ia t ed

    back

    toward

    the

    t r ansmi t t e r i s ca l l ed

    backsca t te r .

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    now smal ler

    than

    the

    order

    of

    a wavelength and the sur face

    cannot be

    cons idered as

    a r e f l ec to r .

    The i n t ens i ty

    of

    a backsca t t e red re tu rn i s ,

    in

    genera l ,

    dependent

    on the

    prope r t i e s of

    the

    sca t t e r e r and the

    sound

    f requency, as well as the range.

    5.5 Noise

    Noise i s

    def ined as

    any

    unwanted s igna l which t ends to

    obscure

    the des i r ed

    echoes

    being

    recorded.

    Several

    types

    and sources of noise wil l

    be

    encountered

    in

    sub-bot tom pro-

    f i l i n g ; most important are background and reverbera t ion noise .

    5 .5 .1 Background

    Noise (See

    Figure

    5-4 of the

    sample

    records)

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    the towing

    sh ip , and

    re su l t s from prope l l e r cav i t a t i on ,

    machinery

    noise

    t ransmi t t ed

    through the hul l , and f low noise .

    Noise

    or ig ina t ing

    from othe r sh ips

    may

    a lso cont r ibute . Flow

    and

    cav i t a t ion

    noise

    tends to

    be broad

    band

    with

    general

    inve rse

    r e l a t ionsh ip

    to

    frequency.

    Machinery noise wil l

    tend

    to

    show

    d i s t i nc t peaks

    a t

    f requencies harmonical ly r e l a t ed

    to

    the

    speed

    of ro ta t ion .

    E l e c t r i c a l noise may

    cont r ibu te to

    the background, al though

    t

    should not

    be

    apparent

    unless

    the

    equipment i s

    improper ly

    grounded.

    Ign i t ion

    noise

    from

    a

    gasol ine

    engine

    or

    60

    z

    hum

    from the power l i n e can

    be

    encountered , and wil l usua l ly be

    e l imina ted by

    proper

    grounding.

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    The s igna l - to -no ise

    r a t i o i s opt imized

    by

    including

    band

    pass f i l t e r in

    the rece iver . This f i l t e r

    passes

    only

    the band

    of

    f requencies

    inc luded in the

    t ransmi t ted

    pulse .

    I t s cent

    e r

    f requency i s the same as the

    c a r r i e r f requency, and i t s

    band

    width

    should

    be inver se ly

    propor t iona l

    to the dura t ion of the

    pulse .

    Thus,

    the noise energy ou t s ide the band necessary to

    accommodate the pulse i s excluded and the s igna l - t o -no i se r a t i o

    improved.

    5 .5 .2 Reverbera t ion Noise

    Reverbera t ion noise

    unl ike

    background

    noise i s

    co r r e l a t ed

    with

    t he t r ansmi t t ed

    pul se

    and sweep r a t e s ince it i s

    the

    r e s u l t of

    backsca t t e red energy or ig ina t i ng a t the

    acous t ic

    pro

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    t h i s poin t ,

    the

    gain s t a r t s to increase

    as

    l i nea r

    funct ion

    of

    t ime

    fo r the

    remainder of the

    sweep. The th resho ld

    value

    of gain and

    the

    r a t e of

    increase are

    ad jus tab le .

    The

    break

    poin t where the gain begins to increase m y

    be

    manually

    ad

    jus ted , or in the

    automat ic

    mode, w i l l t r a ck

    the

    bottom. The

    TV

    r a t e i s

    i dea l l y

    se t to

    compensate

    fo r

    spread ing and

    absorp-

    t i on

    l o s se s in the bottom.

    With

    the

    foregoing

    comments es t ab l i shed , t i s now

    poss ib le to make some

    spec i f i c

    s ta tements

    rega rd ing

    the

    ac tua l

    sub-bot tom

    pr o f i l i ng

    process .

    5 .6 Pene t r a t ion and

    Depth Resolut ion

    In many cases

    the user of

    sub-bot tom

    pr o f i l i ng equipment

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    The

    presen t

    system i s spec i f i c a l l y

    des igned for

    high

    r e so lu

    t i on in

    the upper one or

    two hundred

    f ee t

    of

    sub-bot tom. The

    power l eve l i s

    the maximum achievable a t moderate cos t

    and

    weight

    with

    e l ec t ro - acous t i c

    t r ansducer s .

    Deeper penet ra t ion

    i s

    only

    accomplished

    with

    systems

    using

    lower

    f requencies .

    In

    t h i s

    case ,

    r e so lu t ion i s sac r i f i c ed for

    deeper

    pene t r a t i on .

    Adjustment

    of frequency over the

    range

    3.5 to 7.0 kHz

    and pul se width over wide range a l lows t he use r

    to

    se l ec t

    t he

    bes t

    compromise between

    reso lu t ion

    and

    pene t r a t i on

    for t he

    condi t ions wi th in the c a pa b i l i t i e s o f the equipment .

    5 .6 .2 Pulse

    Energy

    Fur ther

    a f f e c t i n g t he

    r e so lu t ion and pene t r a t ion of

    the

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    5 .6 .3

    Pulse Dura t ion and Rise Time

    co r re l a ry to the r e l a t ionsh ip

    between

    pulse

    dura t ion

    and f i l t e r bandwidth i s t ha t t he r i s e t ime of

    the

    f i l t e r e d

    pul se

    i s

    i nve r s e ly propor t iona l

    to

    the

    bandwidth of the f i l t e r .

    Note

    t ha t

    the

    r i s e

    t ime

    dete rmines

    t he

    r e so lu t ion

    with

    which

    the

    i n s t an t

    of a r r i v a l

    of the pulse may be determined

    while

    the

    pul se dur a t i on

    dete rmines how c lose an

    i n t e rva l between

    two

    pu l se s

    or echoes

    may

    be resolved. Thus as t he pu l se

    energy i s increased provided t he r ece ive r bandwidth i s pro

    pe r ly

    ad jus ted the s igna l - to -no i se

    r a t i o

    w i l l increase and

    more

    pene t r a t ion

    may

    be expected.

    5 .6 .4

    Pene t r a t i on

    Versus

    Resolu t ion

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    By the same token t he un i t

    i s

    i n sens i t ive in

    the

    rece ive

    mode

    to background

    no ise

    from

    d i rec t ions

    widely

    sepa ra t ed

    from the

    ve r t i c a l .

    The

    pa t t e rn of r ad ia t ion

    from the

    t r ansducer

    ar ray

    may

    be

    regarded

    as a

    cone

    whose

    t o t a l

    angle

    i s

    inver se ly

    propor -

    t i o n a l

    to frequency.

    The angle

    var ies

    f rom 55 degrees

    a t

    3.5

    kHz

    to

    30

    degrees a t 7 0 kHz. The beam angle i s def ined ,

    accord ing to s t anda rd prac t i ce , as

    the

    angle between the poin t s

    a t

    a

    f ixed

    dis tance

    from

    t he t ransduce r

    where

    t he

    power i s

    one

    h a l f t he l eve l

    measured

    on the axi s . At wider

    ang les , the

    power

    f a l l s of f sha rp ly , but some energy i s r ad ia t ed beyond

    the

    l i m i t s

    of t he de f ined beamwidth.

    The a rea of t he bottom

    i l l umina ted by the beam i s ,

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    p l us the r e f l e c t i on

    l o s s encountered

    a t

    sub-bot tom hor izons

    o r i n t e r f a c e s w i l l a l so be f ac to r s determining

    the

    ul t imate

    depth of pene t r a t i on . Sca t t e r i ng may

    a l so

    occur in s t r a t a

    t ha t are not pe r f ec t l y homogeneous.

    5 .6 .7

    I l l u s t r a t i v e

    Records

    Figure 5 .1 i s

    a

    por t ion of

    a

    record showing t he e f f ec t

    o f

    a

    bot tom

    where t he r e f l e c t i v i t y i s

    so

    high t ha t no use fu l

    energy

    pene t r a t e s .

    The r eco rd i s of

    a

    t r ave r se

    of

    a

    dredged

    channel . The undredged por t ion a t

    the

    edges of the f igure

    show mul t ip l e

    echoes

    of the bottom

    and

    no

    v i s i b l e

    s t r u c t u r e

    beneath . The mul t i p l e echoes

    a re caused

    by

    second bot tom ;

    t ha t

    i s the echo

    from

    t he bottom

    i s

    r e f l e c t e d

    from

    the

    water

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    '\

    \

    \

    )

    [

    j

    I

    f

    >

    c

    il':

    Q

    i-

    '-".

    t

    r

    fJ

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    t h in l aye r of decaying organic mat ter conta in ing gas

    bubbles

    which

    formed

    a

    b a r r i e r to the sound. Recent dredging, shown

    by the deep pa r t , removed t h i s

    l ayer ,

    a l lowing sound

    to

    pene

    t r a t e .

    The

    depth

    of

    penet ra t ion

    in coarse

    or

    hard-packed

    sand

    or

    grave l wi l l

    be

    l e s s than

    in

    s o f t e r

    mate r ia l s such

    as

    mud

    or silt.

    n

    Figure 5.2

    a t the l e f t -hand

    edge of

    the record ,

    no sub-bot tom l ayers

    are c lea r ly

    v is ib le .

    The

    bot tom

    a t

    t ha t poin t i s sand

    extending to

    a depth beyond the

    capab i l i t y

    of pene t ra t i on .

    The no i se - l ike

    r e t u rn

    extending below

    the

    bot tom

    i s

    probably due to

    sca t t e r ing from gravel

    o r rocks

    mixed with the sand.

    A

    second

    bottom r e t u rn

    i s

    v i s i b l e

    in the

    lower

    l e f t corner .

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    CV )

    I f

    Q

    H

    ; l

    j

    b

    .r {

    I i ;

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    in

    shal low water .

    Figure 5 .4 i s an example of extreme noise condi t ions .

    Under such condi t ions t may appear as a system malfunct ion .

    In t h i s record on the r i gh t s i de the

    noise from the

    sh ip

    complete ly

    obl i t e r a t e s the record

    and no bottom re tu rn

    can

    be

    seen. When the

    ship

    was

    s topped,

    the l e f t

    s ide

    of

    the record ,

    the noise l eve l decreased

    enough

    to

    obtain sa t i s f ac to ry records .

    By changing the pos i t ion

    of

    the towed

    vehic le

    the survey was

    ab le

    to

    cont inue with

    good r e s u l t s .

    Using a hul l mounted ar ray

    with

    16

    t ransducers

    4

    x 4) wi l l

    a l so produce good records

    through

    the hul l of a sh ip

    as can

    be

    seen from

    Figure

    5.5 .

    The hu l l

    should

    be

    hor i zon ta l and

    f l a t

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    6. TROUBLESHOOTING

    Fai lu res

    which

    occur

    in

    the

    system are

    f i r s t i s o l a t e d

    to a par t i cu l a r

    sub-system.

    Then the t roubleshoot ing sec t ion

    of the appropr ia te

    sub-system

    manual can be used to i s o l a t e

    the

    f a i l u r e

    to

    a

    pa r t i c u l a r

    component

    or

    subassembly.

    6.1

    Quick Subsystem Checks Versus

    Symptom

    a .

    Recorder

    w i l l

    not scan.

    Problem i s

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