new design of resistance welding machine

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  • 8/10/2019 New Design of Resistance Welding Machine

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    N e w

    D e s i g n

    of

    R e s i s t a n c e S p o t

    W e l d i n g M a c h i n e

    f o r

    Q u a l i t y C o n t r o l

    BY K.

    I.

    J O H N S O N

    A N D J. C. N E E D H A M

    S i n c e ,

    at a

    g iv e n c u r r e n t

    a n d

    w e ld d u r a t io n ,

    t h e

    e l e c t r o d e lo a d a f f e c t s

    t h e

    f i n a l n u g g e t

    s i z e , t h e

    l o a d v a l u e

    c a n b e

    u s e d

    to

    r e g u l a t e n u g g e t d e v e l o p m e n t

    a n d

    c o m p e n s a t e

    for

    v a r i a t i o n s in e f f e c t iv e h e a t in p u t . W e ld e x p a n s i o n e l e c t r o d e m o v e m e n t a p a r t ) is an

    i n d e x of n u g g e t d e v e lo p m e n t

    a n d c a n

    t h e r e f o r e

    b e

    u t i l i z e d

    a s

    a s u i ta b l e s e n s o r to c o n t r o l

    t h e e l e c t r o d e l o a d

    A B S T R A C T . T he effect of electro de load

    on the growth of the -weld nugget in

    resistance spot welding has been investi

    gated for 0.9 m m (0.03 6 in.) and 1.6 m m

    (0 .064 in . )

    mild

    steel sheet using a

    specially constructed low inertia, r igid

    exper imenta l machine . I t has been shown

    that spot welding can be made to lerant

    to var ia t ions in welding current and t ime

    by automat ica l ly cont ro l l ing the e lec t rode

    load as a function of the weld ex pan sion

    (which is an index of weld nugget de

    v e l o p m e n t ) .

    T he per fo rman ce range of th is self-

    T he authors are associa ted wi th T he Weld

    ing Ins t i tu te . A bington Hal l . C ambridge .

    England .

    load cont ro l has been examined for a

    s imple sys tem in which the e lec t rode

    head is bro ug ht into con tact with the

    work and thereaf ter res t ra ined, so tha t

    as weld expans ion occurs , the e lec t rode

    load increases according to the stiffness

    of the machine f rame ( locked head sys

    t e m . T he result s show tha t und er these

    condi t ions there i s an apprec iable in

    crease in to lerance to var ia t ions in oper

    a t ing current and weld dura t io n .

    T he range of to lerance can be fur ther

    increased by us ing a more complex com

    pound res t ra in t se lf - loading sys tem. T his

    system e mp loys a low init ial st iffness

    which is cons iderab ly increased (with

    expans ion) towards the end of the weld

    per iod . T he res t ra ined head technique

    gives adequately sized welds in spite of

    a we l d i ng c u r r e n t va r ia t i on of + 1 5 % ,

    2 0 , wh i l e no r m a l we l d i ng ma c h i ne

    condi t ions g ive acceptable welds over a

    range of only 1 0 % in 1.6 mm (0 .064

    i n . ) ma t e r i a l . S i mi l a r l y , c ompound r e

    s t ra in t g ives adequate welds when the

    we l d t i me is va r ie d by + 1 0 0 % , 50% ,

    whi le normal opera t ion only g ives ac

    c e p ta b le w e ld s a t + 4 0 % , 2 5 % ( 8

    cycle

    w e l d ) .

    A com pat ib le m oni tor sys tem for weld

    quality assurance is also described which

    util izes the increase in load for the re

    s t ra ined head sys tem to conf i rm tha t a

    nugget has been es tabl i shed .

    T he scope for indus t r ia l appl ica t ion

    of the locked head system is briefly dis

    cussed and designs outlined for obtaining

    locked head charac ter i s t ics on welding

    machines of o therwise convent ional de

    sign.

    122-s | M A R C H 19 72

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    Introduction

    In resistance spot welding, two

    sheets are brought together, held u n

    der pressure between two electrodes

    and a high current passed via the

    electrodes through the workpieces for

    a short time to heat the interface

    sufficiently to form a common weld

    nugget. In normal practice the applied

    load, welding current and weld cycle

    durat ion are preset for a part icular

    applicat ion, depending on the material

    to be welded and on the diameter of

    the electrode t ips . T hese external

    parameters are, as far as possible,held

    constant both from one weld to the

    next and during the formation of any

    one weld. In particular, care is taken

    to ensure that the electrode head

    moves freely in its guides so that the

    electrode load is cons tant and no t

    upset by stiction and the like.

    However, even when the main vari

    ables are held constant, there is often

    considerable variation in weld size or

    quality due to such factors as changes

    in the surface condition of the

    workpieces , electrode wear and the

    shunting effect of alternative current

    paths through adjacent spots . For th is

    reason monitoring the quality of the

    weld or control of the development of

    the nugget is highly desirable. In the

    past, several monitoring techniques

    have been proposed

    1

    and in addition

    in some cases a feedback control has

    been developed in which the moni

    tored parameter is used to sense the

    development of the nugget and to

    operate on one or more of the main

    variables so as to maintain a desired

    nugget size.

    2

    *

    3

    In the weld control

    systems proposed previously the sens

    ing parameter had been arranged ei

    ther to operate on the welding cur

    rent, or to determine the weld cycle

    duration, or both with a substantially

    constant electrode load .

    Owing to the expansion associated

    with the thermal heat ing of the mate

    rial to be welded, including the forma

    tion of the liquid nugget, the welding

    electrodes are, under normal condi

    tions, forced to move apart . T ypically

    using electrode tips 5 mm

    (

    3

    / j

    G

    in .)

    in diameter, this expansion (head

    movement) amounts to about 0 .2 mm

    (0.008 in.) for steel sheets 0.9 mm

    (20 swg) th ick , and about 0 .3 mm

    (0.012 in.) for steel sheets 1.6 mm

    (16 swg) thick.

    T his paper consider s the possibilities

    of controlling the weld nugget by

    means of the electrode load and in

    particular of basing this control on the

    head movement (patents appl ied for) .

    In the s implest arrangement the ex

    pansion directly governs the load ap

    plied, according to the rigidity of the

    welding machine. For th is the elec

    trodes are brought together into con

    tact with the work, and then locked or

    restrained to prevent their free move

    men t apar t . T he a t t empted expans ion

    of the weld nugget then results in a

    corresponding increase in the applied

    load . T his is termed a ' locked head '

    system to differentiate it from conven

    tional resistance welding equipment in

    which the moving electrode is rela

    tively free.

    Principle of Automatic Weld

    Correction by Electrode Load

    Effect of Load on Nugget Formation

    T he new correct ion m ethod is based

    on automatical ly varying the electrode

    load during the weld cycle and in

    02-

    5

    0-75

    S010

    < 3

    005

    6

    ta

    5S2

    /

    0

    L 0

    Splash

    Normal

    Electrode tip dia47 mm 0-18in.)

    Transformer tap 4,

    3-3Vo.c. approx.

    6-OkA)

    Weld duration 0-18 sec 9 cycles at 50 Hz)

    ^

    i

    I

    I

    0-5

    / 7-5

    Electrode force, kN

    IFace

    I fracture

    I

    l

    I

    700 200 300

    Electrode force, Ibf

    400

    500

    Fig. 1Effect

    of electrode load on nugget diameter for 0.9 mm (20 swg) mild steel

    W E L D I N G R E S E A R C H S U P P L E M E N T I

    123-s

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    particular with controlling the load as

    a function of the development of the

    nugget by means of the associated

    expansion . T hat the electrode load or

    pressure is significant in resistance

    spot welding is well known and for

    consistent welds in mild steel it has

    been recommended that the pressure

    be maintained constant with in

    15 .

    3

    T hus for a g iven material and

    thickness , part icular combinat ions of

    weld current and durat ion are es tab

    lished by trial and error for a prede

    termined electrode load which itself is

    based on the tip diameter which in

    turn is related to sheet thickness.

    T he effect of variation in electrod e

    load on nugget development with oth

    erwise constant welding conditions is

    illustrated in Fig. 1 for 0.9 mm (20

    swg) mild steel. [In these tests the

    degree of phase shift (heat control) is

    constant but the current can be varied

    by altering the t ransform er tap .] T he

    current at a given voltage tap setting

    is nominally constant but does in

    crease by 2 to 3% from a low to a

    high electrode load owing to the de

    crease in in terfacial res is tance.) A t a

    given current and weld duration the

    nugget size increases with decrease in

    electrode load until weld splashing

    occurs ; while on the o ther hand with

    increase in load the nugget size de

    creases until a face fracture sets in.

    With further increase in load the nug

    get size rapidly becomes insignificant

    resulting in a stuck weld which has no

    strength .

    T he mechan isms by which electrode

    load affects the nugget development

    are believed to be threefold. First,

    with increase in load the interfacial

    resistance decreases and hence the

    initial heating at the interface is re

    duced at the early stages of the weld

    dura t ion .

    5

    Secondly the electrode con

    tact with the work is improved at

    higher loads and the current distribu

    tion from the electrode tip into the

    workpiece is modified giving a lower

    current densi ty and hence a reduced

    effective heating. Finally, particularly

    with thin sheet, the increased elec

    trode load results in increased heat

    conduct ion from the workpiece to the

    water-cooled electrodes .

    T hese three factors act in the same

    direction and hence the nugget de

    velopment is reasonably dependent on

    the electrode load . T hus , as shown in

    Fig. 1, the change in nugget diameter

    with load is approximately linear be

    tween the limits where weld splashing

    sets in and where the nugget decreases

    very rapidly in size to leave a low

    strength or face fracture condition. In

    this case a change of 25% in elec

    trode load results in a 10% change in

    nugget diam eter for a well develope d

    nugget which is approximately the

    same size as the electrode tip.

    S imi la r nugge t d iameter / e lec t rode

    load relations can be found for other

    welding currents, as shown in Fig. 2

    for 0.9 mm (20 swg) mild steel. In

    this case the weld heat is altered in

    relatively large steps by changes in the

    transformer primary tapping, g iv ing

    open circuit voltages ranging from

    4.1v to 2 .8v or broadly + 2 5 % to

    1 5 %

    of the normal condition

    ( t rans fo rmer t ap 3 .3v ) . A s can be

    seen from Fig. 2 there is a correction

    zone for 0.9 mm (20 swg) mild steel

    where, in spite of current changes

    from about 5ka to 7ka, a substantially

    0-2

    0-75

    0-70

    3 *

    Splash

    Compound compliance

    075kN 170 Ibf)

    initial force

    Free electrode

    2 3 kN

    500 Ibf)

    force

    Weld duration 0-16 sec

    8 cycles at 50 Hz)

    Electrode tip dia. 64mmfAin.)

    8

    Current, kA

    10

    11

    12

    03

    r

    8

    02

    c

    0-7

    6

    ri

    *~

    cu

    c

    T

    Compound compliance

    075kN 170 Ibf)

    initial force

    x

    -

    T

    *

    I

    o - ^ o Splash

    Free electrode

    23 kN 500 Ibf) force

    Welding current 9-4 kA

    b)

    10 12 14

    Time, cycles at 50 Hz

    16 18 20

    Fig.

    fjNugget growth in 1.6 mm (16 swg) mi ld steel with free and co mpou nd com pliance restrained electrode systems: (a)

    effect of weld current on nugget diameter for constant weld durat ion; (b) effect of weld t ime on nugget diameter for constant

    current

    distinctive with the dual or compound

    spring rate system as evidenced by the

    results given in Fig. 6a and 6b as well

    as by the table on performance

    toleran ce. T he principal feature in this

    system is that the initial load is itself

    low as well as having initially a low

    spring rate. T he design of the elec

    trode support to give initially a suffi

    ciently free movement is simple. For

    example a small degree of free move

    ment can be provided in the locking

    system itself or the electrode support

    can include a thin pad of rubber or

    other soft material or a flat spring

    B elleville type washe r to give the de

    sired low spring rate.

    T he higher sp ring rate is then

    provided by the complete locking of

    the electrode or by ensuring that the

    piston is suitably jammed. One method

    of preventing free movement of the

    piston is to use a hydraulic ram in

    which th e fluid circuit is closed dur ing

    the welding operat ion . A ny reverse

    movement of the electrode tends then

    to compress the hydraulic fluid (which

    has a spring rate of the order of 15

    N / m m

    2

    (2000 psi) for a 1% com

    pression by volume) and hence in

    creases the electrode loading.

    T he degree of com pound compli

    ance can also be readily provided in

    an all hydraulic system by adding a

    small freely compressible capsule in

    the hydraul ic circuit . T he basic ar

    rangements for an hydraulically actu

    ated electrode are shown diagrammat-

    ically in Fig. 7b in which a limited

    W E L D I N G R E S E A R C H S U P P L E M E N T

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    Hydraulic brake

    calipers

    a

    Electrode^^

    assembly I J

    Adjustable stop

    Spring

    Hydraulic fluid

    Solenoid valve

    Clamp

    From

    timer

    y//////////////////^ Retract

    Fig. 7Schematic

    diagrams

    of

    systems

    for

    locked head operat ion:

    a)

    restrained

    electrode by external c lam p; b) compound compl iance us ing hydraul ic ram

    degree

    of

    free reverse movement

    is

    permit ted

    by the

    small expansion bel

    lows

    on the

    high pressu re side

    of the

    cyl inder . Here the locking is provided

    by

    the

    solenoid valve w hich

    is

    con

    trolled

    via the

    weld t ime r .

    Wi th

    the

    com pound res train t

    the

    initial load that is usedis low,typical

    ly between 25 and 50 of normal

    levels,

    so as to

    encourage nugget

    de

    velopment

    at an

    early stage

    in the

    weld cycle. Weld splash,

    however,

    is

    prevented by the ensuing high spring

    rate which prevents over-development

    of

    the

    nugget

    as

    already described.

    It

    is this combination

    of low

    initial load

    and virtually free head together witha

    high final load, fixed head

    (as a

    func

    tionof theexpansion) which resul tsin

    the wide tolerance

    to

    variat ions

    in

    heat input (welding current)

    and

    weld

    durat ion, shown

    by the

    nugget size

    datain Fig. 6.

    Automatic Weld Quality Monitor

    A s already discussed,

    the

    control

    of

    nugget development

    by

    electro de load

    is feasible and it involves a relatively

    large change of electrode load to be

    effective. A lso the load change is di

    rectly caused

    by the

    weld expansion .

    N ow

    it has

    been established previously

    that there is a good correlation be

    tween head movement (expansion)

    and weld quality (since the head

    movemen t

    is a

    direct indication

    of the

    nugget deve lopmen t ) . Hence

    the ex

    pansion measurement can beused as a

    monitor

    of

    weld qual i ty

    7

    al though

    there

    is the

    basic practical difficulty

    of

    registering such small movements in

    industry, particularly on portablema

    chines .

    T his difficulty

    is

    circumvented

    in

    the restrained electrode system, since

    in effect the load c hange serves as a

    measure

    of the

    head movem en t

    ob

    t a ined . Thu s

    the

    electrode assembly

    forms

    a

    cal iper

    by

    which

    to

    register

    the weld expansion

    and if the

    elec

    trode actuation point (or effective

    cal iper fu lcrum)

    is

    locked

    or re

    strained from free movement then

    the

    stress developed

    in the

    locking system

    corresponds directly with expansion.

    It should be noted that the load

    change is large and can be readily

    detected especially with the hydraul ic

    type

    of

    loading/ locking system. A lso ,

    since with

    the

    locked head w ith du al

    compliance the system is essentially

    tolerant then only a relatively simple

    weld quality monitorisneeded (viz,to

    detect that

    the

    load increased signifi

    cantly from

    the low

    in i tial level) . T his

    corresponds to the formation of the

    weld nugget which as already de

    scribed develops early

    in the

    weld

    cycle

    and

    then

    is

    held from splashing

    by

    the

    increase

    in

    electrode load.

    T h u s

    for

    critical weld applications

    not only does the res trained electrode

    system provide a greater degree of

    reliabilitydue to itsinherent to lerance

    to variations

    in

    effective w eld he atin g

    bu t

    it

    provides also

    a

    ready means

    for

    weld quality assurance.

    T ests have shown that this simple

    monitor

    of the

    response

    of the re

    strained electrode correctly registers

    which welds have well established

    nuggets for a variety of external devi

    ations

    in the

    welding condit ions ,

    in

    cluding change

    of

    current , weld dura

    tion initial electrode load

    and tip

    diameter (for truncated cone elec

    trodes) either singly or in any combi

    nat ion .

    It

    also registers correctly

    for

    shunted welds even

    in the

    ex t reme

    case of a spot placed between two

    previous spot welds. The only limita

    tion is that of a weld at the very edge

    of

    the

    sheet which collapses w ithout

    expansion

    and

    expels without increase

    in load . Here the monitor indicates a

    suspect weld (pressure failing to in

    crease) even though a nugget was

    formed before

    it

    splashed .

    Applicationof Restrained

    Electrode Systems

    In

    the

    work reported

    a

    relatively

    rigid spot welding machine

    has

    been

    used

    in

    which

    the

    degree

    of

    restraint

    with a locked head ishigh . T his condi

    tion applies also to s tandard bench or

    fixed station resistance welding

    ma

    chines

    in

    which

    the

    moving electrode

    is carried directly

    by the ram and is

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    not par t of an extension arm . T he

    system could also be applied to por

    table spot welding guns so long as the

    electrode

    support arms are relatively

    short or of such a construction that a

    reasonably rigid system is achieved. In

    this connection it is noted that a load

    change of at least 30% with weld

    expansion is required .

    T he rest ra ined e lec t rode system

    should be applicable to roll spot seam

    welding but with the addition of some

    means for compensating for longer

    term varia t ions such as wheel eccen

    tricity and wear. For this a hydrauli-

    cally

    actuated head would be suitable

    since it could provide both the long

    term free electrode mechanism and

    the short term restrained electrode

    effect . For example , the hydraul ic ram

    could be pressurized by an air cylinder

    so as to main tain a long term mea n

    load which would allow the system to

    follow variations in sheet thickness or

    in wheel radius . However , by provid

    ing a constriction in the hydraulic

    supply, the short term head movement

    would be restrained and cause a cor

    responding increase in pressure in the

    hydraulic fluid which in turn increases

    the electrode load.

    T he system should a lso be appl ica

    ble to stitch welding but in this case it

    may not be necessary to incorporate a

    dual compl iance rest ra int . Th is ar ises

    since there is a stage of negligible

    head movement or even slight collapse

    during the initial part of a sti tch weld

    before a positive expansion is regis

    tered . This m ay be due to the overlap

    of spots whereby the new spot falls on

    the shoulder or edge of the indenta

    tion produced by the previous spot .

    T he deta i led mech anism is not known

    but i t is believed that the shoulder

    initially collapses and offsets the ex

    pansion until a nugget is developing at

    the new point . For the remainder of

    the weld cycle a positive head move

    ment is registered and with the re

    strained electrode system this would

    result in an increasing electrode load

    to contain the nugget as already de

    scr ibed.

    For both sti tch welding and roll

    spot seam welding, the weld could also

    be mo nito red *in term s of the in creas e

    in electrode load arising.

    Finally it is believed that this new

    concept in machine design for resist

    ance welding

    will

    lead to a greatly

    increased confidence in this, the

    oldest, electric welding process for

    crit ical applications such as in the

    aerospace industry and for the struc

    turally important welds in the auto

    mobi le mass product ion indust ry . T he

    increased tolerance in operation and

    the faoility for weld quality assurance

    has been clearly demonstrated for

    mild steel sheet and these advantages

    are expected to apply also to the wide

    range of materials which are currently

    resistance welded by the conventional

    process .

    Conclusions

    1. Since at a given current and

    weld durat ion the e lec t rode load

    affects the final nugget size, the load

    can in principle be used to

    reguLate

    the nugget development and to com

    pensate for variations in effective heat

    input due (for example) to changes in

    current . T he e lec t rode movem ent

    apart (weld expansion) which is an

    index of the nugget development

    provides a suitable sensor for control

    of the load.

    2. For weld correct ion during the

    weld period, in the simplest arrange

    ment the electrode movement is react

    ed against a rigid support so that the

    electrode load increases considerably

    with expan sion accord ing to the

    stiffness (spring rate) of the support .

    On a r igid bench w elding m achine

    (fit ted with stops to prevent move

    ment of the electrode head with re

    spect to the machine frame after the

    workpiece is c lamp ed) the tolerance

    to

    changes

    in weld current , though

    limited, is twice that for the norm al

    free system.

    3. T he restra ined e lec t rode system

    is applicable to many types of resist

    ance welding machine but the max

    imum spring rate obtainable is l imited

    by the stiffness of the electrode sup

    port system especially with portable

    welding machines .

    4 .

    With a compound spring ra te

    (giving initially a low degree of re

    straint followed by a high stiffness) the

    weld tolerance is greatly increased

    over that from a convent ional ma

    chine with a nominally free electrode

    head. T he nugget diame ter for 1.6

    mm (16 swg) mild steel is main tained

    at about 6 1 mm (0 .25 0 .04

    in . ) for current var ia tions of + 1 5 % ,

    20%

    and (a t the correct cu rrent)

    for time varia t ions of 50% ,

    + 10 0% . A bnorm al ly low init ia l e lec

    trode loads are used so that the nug

    get is established early in the weld

    cycle without splashing but thereafter

    its further deve lopm ent is inhibited by

    the dampening effect of the rapidly

    increasing e lec t rode load.

    5.

    T he restra ined head provides a

    means for registering the expansion of

    the weld by the increased load and

    hence serves as a monitor of weld

    quality since, except for a weld at the

    sheet edge, the nugget formation is

    c losely corre la ted wi th expansion. T he

    load moni tor reads correct ly for var i

    ations in current, weld duration, elec

    t rode size and for shunted welds .

    Since the dual compliance system is

    essentially tolerant, this results in sat

    isfactory welds even with major chang

    es in welding conditions.

    6 . The combina t ion

    of

    the re

    strained electrode approach with its

    monitor facili ty is recommended for

    weld

    quality assurance in crit ical spot

    welding applications for both the

    aerospace and mass product ion indus

    tries.

    cknowledgements

    T he authors express thei r thanks to

    the Director General of the Welding

    Institute for permission to publish this

    paper and to thei r col leagues M.D.

    Hannah and R . G . Newl ing who were

    responsible for the experimental data

    and machine design.

    References

    1. R o d e n . W . A . , E v a l u a t i o n o t R e s i s t

    a n c e W e l d i n g I n - P r o c e s s M o n i t o r s .

    Weld-

    ing Journal,

    V ol . 47 . N o .

    11 .

    pp. 515-s to

    521-s, 1968.

    2 . G r a n t . W . A . . E v a l u a t i o n o f E l e c

    t r o n i c M o n i t o r e d R e s i s t a n c e W e l d i n g C o n -

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    563-567. 1962.

    3. O r l o v .

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    Svarka,

    V ol . 21 . N o . 6 . pp . 50 - 54 . 1968 .

    4 . B e a t s o n . E . V . , T e c h n i q u e s f o r S p o t

    W e l d i n g L o w C a r b o n S t e e l w i t h T r u n c a t e d

    C o n e E l e c t r o d e s . I n t e r n a t i o n a l I n s t i t u t e

    of Wel di ng D oc . 111-283-66. 1966.

    5 . N i c h o l s o n . S . a n d A p p s . R . I . . . H e a t

    B u i l d - u p a n d W e l d N u g g e t F o r m a t i o n i n

    M i ld S t e e l S p o t W e l d s . A d v a n c e s in W e l d

    i n g P r o c e s s e s C o n f e r e n ce .

    H a r r o g a t e ,

    W e l d

    i n g I n s t i t u t e . 1 9 7 0 .

    6 . E v r a r d . M . a n d H a s l e . E . . R e s i s t

    a n c e W e l d i n g P a r a m e t e r s ,

    British Weld-

    ing Journal,

    Vol . 5 , No . 1 , pp . 18-20, 1958.

    7.

    W a l l e r . D . N . a n d K n o w l s o n . P . M . ,

    E l e c t r o d e S e p a r a t i o n A p p l i e d to Q u a l i t y

    Conti'ol

    in R e s i s t a n c e W e l d i n g ,

    Welding

    Journal,

    Vol . 44 . No. 4 . pp . 168-s to 174-s.

    1965.

    APRIL IS

    NATIONAL

    WELDED

    PRODUCTS < / I

    MONTH

    VISIT

    THE A.W.S.

    WELDING

    SHOW

    W E L D I N G R E S E A R C H S U P P L E M E N T

    131 s