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    Development o f Fil ler Metals

    and

    Procedures fo r

    Vacuum

    Braz ing

    o f

    Alum inum

    S e v e r a l b r a z in g f il l e r m e t a l c o m p o s i ti o n s h a v e b e e n d e v e lo p e d

    w h i c h o f f e r s i g n i f ic a n t im p r o v e m e n t s o v e r e x i s t in g c o m p o s i ti o n s

    T h e y b r a z e in v a c u u m

    at

    t e m p e r a t u r e s l o w e r t h a n n o r m a l f l o w

    t e m p e r a t u r e s a n d h a v e e q u a l o r b e t t e r f lo w a b i l i t y

    B Y W. J . W E R N E R , G. M . S L A U G H T E R A N D F. B . G U R T N E R

    Introduction

    This report documents work per

    formed toward the development of

    new brazing filler metals for vacuum-

    fluxless brazing (1 X

    1 0 ~

    6

    to r r )

    certain aluminum alloys of interest to

    the Army. The base metals under

    considerat ion were al loys 6061, 2219,

    7075 and 2024. Brazing filler metal

    flow temperatures needed for these

    al loys encompass the temperature

    range 900 to 1200F. Specifically, the

    contract called for the development of

    alloys with flow temperatures of 950,

    1000,

    and 1050F . Final ly , corrosion

    compatibility of the brazing filler met

    al with certain chemical agents was

    necessary and to this end a survey of

    potent ial ly compatible elements com

    piled by the contractor was utilized.

    We began the invest igat ion with a

    survey of the l i terature. Unfortunate

    ly, there is very little published work

    on fluxless-vacuum and/or inert gas

    brazing of aluminum. M. M.

    Schwar tz

    1

    et al showed the feasibility

    of vacuum fluxless brazing production

    quanti t ies of aluminum al loy 6061

    containers of helium leaktight quality

    by closely controlling process parame

    ters using a commercial brazing filler

    metal . Brazing al loy No. 718 (nomi

    nal ly 88% aluminum, 12% si l icon)

    was used. This alloy is widely used

    commercially for both dip and fur

    nace brazing and is available in both

    wire and foil form. As might be ex

    pected, the success of the endeavor

    was largely due to the use of laborato-

    MESSRS. WERNER and SLAUGHTER are

    with the U.S. Atomic Energ y Comm ission.

    Tenn. which is operated by Union Carbide

    Corp. MR. GURTNER is with the Dept.

    ot the Army, Technical Support Directo

    ra te .

    Industrial Operations Div., Edge-

    wood Arsenal , Md.

    ry cleanliness levels under production

    condit ions. The maximum al lowable

    lag between cleaning and brazing was

    found to be 12 hours.

    C. S. Beuyukian

    2

    developed tech

    niques for vacuum or inert gas fluxless

    brazing of aluminum cold plates for

    use in Apollo command modules . In

    this work, brazing filler metal No. 718

    and No. 23 brazing sheet were evalu

    ated. Alloy No. 718 is nominal ly 88%

    aluminum , 12 % si l icon; No .

    23

    b raz

    ing sheet is comprised of 6951 base

    alloy clad on one side with 4045

    brazing filler

    metalnominally

    9 0 %

    aluminum, 10% si l icon. Base metals

    6061 and 5052 were considered for

    the main body of the assembly.

    In general, better results were ob

    tained using vacuum. The techniques

    developed are unique in that stringent

    flatness requirements placed on the

    assembly by design required that braz

    ing operat ions be performed in heated

    platen presses at moderate pressures.

    The use of pressure during brazing

    undoubtedly influenced oxide penetra

    t ion and/or displacement during the

    brazing operat ion. Product ion brazing

    was carried out in the temperature

    range 1055 to 1095F using brazing

    times of at least 10 minutes.

    Under these condit ions, aluminum

    alloy 6061 was preferred over 5052

    because alloy 5052 exhibited a greater

    suscept ibi l i ty to in tergranular penetra

    tion by silicon. Use of alloy 5052

    would therefore have required more

    rigid t ime- temperature control during

    the brazing cycle. In addition, silicon

    diffusion resulted in embrittlement of

    5052.

    No . 23 brazing sheet was chosen

    for product ion over the combinat ion

    of brazing al loy Nos. 718 and 6061

    for both metallurgical and process ad

    vantages. As a single entity, it was

    immediately more desirable from a

    cleaning, assembling and material

    handling s tandpoint . Metal lurgical ly ,

    the 4045 brazing filler metal with its

    lower silicon content allowed greater

    lat i tude in processing parameters than

    did alloy No. 718.

    Final ly , the workers at Aeronca,

    Inc. completed a study on inert gas

    brazing of aluminum in early 1967.

    3

    Their work was concerned with de

    velopment of h igh s trength brazed

    aluminum honeycomb structures

    which would withstand a range of

    cryogenic (423F) through elevated

    (600F) temperatures . All of the base

    metals involved in the s tudy, X7005,

    X7106, and 7039, began to melt with

    in the range of 1080 to

    1120F.

    As a

    resul t , a 1050F maximum flow tem

    perature for the brazing filler metal

    was needed.

    Three commercial brazing al loys

    were evaluated in combinat ion with

    the aforementioned base metals

    716, 718, and 719. Nu mb er 716 con

    ta ins nomina l ly 86 % a luminum, 10%

    sil icon, and 4% copper; 718 contains

    nominal ly 88% aluminum, 12% si l i

    con; and 719 contains nominal ly 76%

    aluminum, 10% si l icon, 10% zinc and

    4 % copper. I t was found that the

    aluminum-silicon brazing alloys per

    formed best as claddings.

    The researchers developed several

    new brazing filler metals during the

    course of their investigation. Two in

    part icular showed promise. Both al

    loys had a base composi t ion of 68%

    aluminum, 7% si l icon, 15% germani

    um; their compositions were modified

    with 10% zinc, and 10% si lver, re

    spectively. Both alloys brazed at

    1020F. These new al loys looked espe

    cially good in combination with

    64-s ] F E B R U A R Y 1 9 7 2

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    Table

    1Nominal

    Composit ions,

    A l lo y d e s i g n a t i o n

    6061 ( l im i t i n g )

    6061 (n om i na l )

    2219

    1

    ( l i m i t i n g )

    2219

    2

    ( n o m i n a l )

    7075

    ( li m i t i n g )

    7075 ( n o m i n a l )

    2024 ( l im i t i n g )

    2024 ( no m i na l )

    .

    Si

    Li

    0.40-0.8

    0.6

    0.20

    0.40

    0.50

    mits

    and Melt ing Ra

    Fe

    0.7

    0.30

    0.50

    0.50

    Cu

    0.15-0.40

    0.27

    5.8 -6.8

    6.3

    1.2 -2.0

    1.6

    3.8 -4.9

    4.4

    n g e s of Alloys Under Con

    - C o m p o s i t i o n

    M n

    0.15

    0.20-0.40

    0.30

    0.30

    0.30-0.9

    0.6

    w e i g h t p e

    M g

    0.8 -1.2

    1.0

    0.02

    2.1 -2.9

    2.5

    1.2

    -1.8

    1.5

    sideration

    Cr

    0.04-0.35

    0.20

    0.18-0.35

    0.30

    0.10

    Zn

    0.25

    0.10

    5.1 -6 .1

    5.6

    0.25

    T i

    0.15

    0.20-0.10

    0.06

    0.20

    A p p r o x i m a t e

    -,

    m e l t i n g

    r a n g e ,F

    1080-1200

    1080-1200

    1010-1190

    1010-1190

    890-1180

    890-1180

    935-1180

    935-1180

    1

    V a n a d i u m 0 . 0 5- 0. 15 , z i r c o n i u m 0 .1 0- 0. 25

    -

    V a n a d i u m 0 .10 , z i r c o n i u m 0.18

    X 7 1 0 6 . Alloy 719 remained the num

    ber one choice for brazing X7005.

    M a t e r i a l s

    Table 1 shows the nominal com

    positions and compositional limits of

    the base metals under consideration in

    the program, along with their melting

    ranges. Joining of alloys 6061 and

    2219 is accomplished industrially by

    dip or furnace brazing techniques both

    of which employ liberal amounts of

    flux. In addition, alloy 6061 has also

    been brazed without flux using vacu

    um and/or inert atmospheres .

    1

    *

    2

    A s

    a result, good cleaning and handling

    procedures are not a problem with

    these two alloys. In fact, cleaning

    procedures are available in the Metals

    and Ceramics Division for both of

    these alloys since they are routinely

    hot roll-bonded into dispersion type

    fuel plates using standard picture

    frame techniques.

    Alloys 7075 and 2024, on the other

    hand, are not considered brazeable

    using established commercial tech

    niques and commercial brazing filler

    alloys. In the first place, both alloys

    have melting points below the flow

    temperatures of the commercial braz

    ing filler metals (Table 1 ) . Secondly,

    both al loys contain appreciable

    amounts of magnesium (2.5 and

    1.5%, respect ively). Normally , al loys

    with magnesium contents greater than

    2 . 0 % are considered difficult to braze

    industrially; and alloys with magnesium

    contents greater than 2 .5% are con

    sidered unbrazeable. This is due to the

    fact that state-of-the-art fluxes do not

    remove the tenacious oxides formed

    on these alloys.

    E q u i p m e n t a n d E x p e r i m e n t a l

    P r o c e d u r e

    The vacuum furnace apparatus for

    flow temperature and wettabi l i ty de

    terminations is shown in Fig. 1. The

    system is capable of maintaining a

    vacuum of 1 X

    10 ~

    r>

    torr at brazing

    temperature. The picture shows the

    furnace rolled back off the muffle. In

    a typical brazing cycle the specimen is

    placed into the cold muffle. After

    pump-down, the heated furnace is

    rolled onto the muffle, and the work

    very rapidly comes to temperature.

    After holding for the proper brazing

    t ime, the furnace is rolled off the

    muffle. Simultaneous with the former

    operat ion, hel ium can be admit ted to

    facilitate rapid cooling or quenching

    of the test assem bly. Diffusion effects

    can probably be limited by both of

    these operations.

    A typical t ime- temperature re

    sponse curve for the furnace is shown

    in Fig . 2 ; the temperature measure

    ments indicated are those of an actual

    sample. Chromel-P versus alumel

    thermocouples were at tached to a

    specimen and temperature measure

    ments were made using a potent iom-

    1

    ' :.

    ';..:

    \

    '

    * ( & -

    t

    i

    ' * ~ * i

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    Table 2-

    -List of Potentially Compatible

    Metal

    Alloy Formulation

    Ele

    m e n t

    Al

    A m

    Sb

    Ba

    Be

    B

    Ca

    Ce

    Cr

    Cu

    D y

    Er

    Ge

    A u

    Hf

    In

    Ir

    Fe

    Li

    M g

    M n

    M o

    Nd

    Ni

    Nb

    Os

    P d

    P t

    P r

    Re

    Rh

    Ru

    Sm

    A g

    Ta

    Te

    Th

    T i

    V

    Yb

    Y

    Zr

    P o t e n t i a l ,

    v o l t s

    -1 .706

    +0.212

    - 2 . 9 0

    - 2 . 7 6

    -2 .335

    - 0 . 4 1

    +0.158

    +1.42

    - 0 . 4 9

    +0.777

    -3 .045

    -2 .375

    -1 .029

    -2 .246

    - 0 . 2 3

    +0.344(?)

    +0.7966

    +0.593

    - 2 . 0

    -0 .255

    Elements for Brazing Filler

    Supplied by Edgewood Arsenal

    M e l t i n g

    po i n t , F

    1220.4

    1562

    1166.9

    1317

    2460/2640

    3690

    1540

    1495

    3407

    1981.4

    2565

    2727

    1719

    1945.4

    4032

    313.1

    4449

    2799

    1688

    357

    1202

    2273

    4730

    1866

    2647

    4474

    4900

    2826

    3217

    1686

    5755

    3571

    4530

    1962

    1760.9

    5425

    842

    3182

    3035

    3450

    1515

    2723

    3366

    B o i l i n g

    p o i n t ,F

    4442

    2516

    2980

    5378

    2908.6

    6278

    4829

    4703

    4226

    4766

    5125

    5380

    9750

    3632

    9570

    5432

    6276.2

    2426

    2025

    3900

    10,040

    5756

    4950

    8901

    9950

    7200

    8185

    5468

    10,650

    8130

    4900

    2966

    4010

    9800

    1813.6

    6332

    5900

    6150

    2786

    5800

    6470

    S pe c i f i c

    g r a v i t y

    2.6989

    11.7

    6.691

    3.5

    1.848

    2.34

    1.55

    8.23/6.67

    7.18-2

    8.96

    8.526

    9.051

    5.323

    19.32

    13.29

    7.31

    22.42

    7.874

    5.98/5.186

    0.534

    1.728

    7.21/7.44

    10.22

    6.80/7.004

    8.902

    8.57

    22.57

    12.02

    21.45

    6.6/6.7

    21.02

    12.41

    12.41

    7.5/7.4

    10.50

    16.6

    6.24

    11.66

    4.54

    6.11

    6.977

    4.45

    6.35

    S o l i d

    s o l u b i l i t y /F *

    0.1 /1232.6

    0.05 /1166

    0.00190/1190.86

    2.8770/1108.8

    0.61%/1166

    4.10%/932

    1.22%/1223.6

    13 /1173.2

    0.052 /1211

    0.0370/1121

    5.2 /

    11.5 /752

    1.35%/1158.8

    0.040 /1157

    0.1%/1139

    0.1 /1215.5

    0.1 /1218.2

    Eu t e c t i c 28

    0.1 /1173.2

    1-1.5%/1220

    0.6 /1224.5

    0.1 /1191.2

    0.28 /1220

    * P e r c e n t a t t e m p ( F ) .

    C O MP O S I T I O N (>%)

    1

    1 Z

    BOO

    5

    4 0 0

    In

    /

    ...

    tst

    --.

    S

    F i g .

    3Ternary

    plo t o f t h e Al-Si-ln s y s t e m w i t h a t t a c h e d

    b in a r y p ha s e d ia g r a m s fo r e s t i m a t i n g c o m p o s i t io n s o f p o t e n

    t i a l i n t e r e s t t o p r o g r a m

    ployed, care is taken to reduce the

    oxide th ickness to a wo rkab le mini

    mum before flux is applied.

    The consensus on the mechanism of

    flux action is as follows: First, as the

    assembly is brought to brazing tem

    perature the oxide film

    microfissures

    due to the differences in coefficients of

    thermal expansion between the oxide

    and base metal . Flux readi ly enters

    these microfissures and undermines

    the oxide to some extent. If the oxide

    is

    workably

    thin , i t breaks up during

    the undermining process . This contin

    ues until the flux is consumed or the

    metal surface is cleared of oxide.

    In fluxless brazing, we must assume

    that , as in commercial operat ions, a

    workably thin oxide film is microfis-

    sured during heat-up to the brazing

    tempera tu re . Undermin ing o f the ox

    ide in the fluxless process must be due

    to the action of the brazing filler

    me tal. It is note wo rthy th at diffusion

    (over short d is tances) may play an

    important role in the fluxless brazing

    process . Rate of heat ing to brazing

    temperature is also a factor of major

    importance s ince oxidat ion of alumi

    num takes place in the best vacuums

    and/or inert atmospheres . In addit ion,

    faster heating rates may affect the

    degree of oxide microfissuring. In any

    event, there is a multiplicity of factors

    to consider which probably will affect

    the vacuu m brazing of aluminu m.

    Both 6061 and 2219, as well as all

    the experimental brazing filler metals,

    were cleaned by immersion in to a 20

    vol%HN0

    8

    2 vol %HFwat er

    solu

    t ion at room temperature. The clean

    ing step was followed immediately by

    a cold water r inse which, in turn , was

    followed by flushing with acetone. Al

    loys 2024 and 7075 did not respond to

    the aforementioned chemical cleaning

    process to our satisfaction. Both alloys

    did, however, respond to a low-

    temperature perchloric acid electropol-

    ishing t reatment .

    In our very first experiments we

    noted that test results were influenced

    by the t ime span between cleaning and

    brazing. As a result, we held the time

    between cleaning and brazing to a

    max imum of 1 hour w hich, al though

    possibly somewhat difficult for pro

    duct ion work, was fel t to be opt imum

    for experimental brazing filler metal

    evaluat ion.

    Brazing Alloy

    Development

    Experimental brazing fi l ler metal

    composi t ions were formulated using

    binary phase diagram information to

    est imate the behavior of ternary al

    loys. A list of potentially compatible

    elements compiled by the contractor

    was used as a guide (Table 2) but it

    was not utilized absolutely since this

    would have seriously limited the choice

    66-s i F E B R U A R Y 1 97 2

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    1600

    800

    G60

    400

    A.

    ?=*

    C O M P O S I T I O N (wl ?

    2 0 4 0 6 0

    ^

    v?

    u

    BO

    S

    - , . J :

    T~

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    F i g .

    7Macro

    of p a d t e s t w i t h Al-Si-ln A l lo y N o . 8 v a c u u m

    b razed f o r 7 m i nu t es a t 1075F

    F i g . 9 M ac r o o f p a d t e s t o n A l - S i -l n a l l o y N o . 6 v a c u u m

    b r a z e d f o r 7 m i n u t e s a t 1 085F . N o t e e x c e s s i v e f i l l e r m e t a l -

    ba s e m e t a l r e a c t i o n

    F i g . 10T-joint braze d w i th A l -S i - ln a l l o y No. 6 a t 1085F for

    5 m i n u t e s

    F i g .

    8Micro

    of i n t e r f ac e be tween 6061

    bas e m e t a l a n d N o . 8 A l - S i - ln a l l o y .

    M a g :250X

    Table

    4

    Flow

    Temperatures and

    Compositions of the

    Al-Si-Ge

    Alloys

    F low

    A l l o y C o m p o s i t io n , w t . t e m p ,

    n u m b e r Al Si Ge F

    1

    2

    3

    4

    5

    6

    7

    8

    9

    10

    11

    12

    55

    55

    55

    55

    45

    45

    45

    45

    35

    35

    35

    35

    5

    10

    15

    20

    5

    10

    15

    20

    5

    10

    15

    20

    40

    35

    30

    25

    50

    45

    40

    35

    60

    55

    50

    45

    1020

    1060

    1060

    1065

    1020

    1060

    1065

    1095

    1020

    1065

    1075

    1075

    filler metals are quite close to the

    melting points of the base metals. The

    same alloy was subsequently used to

    braze the T-joint shown in Fig. 10

    using a slightly shorter brazing cycle

    with obviously much improved results.

    Our experience indicates that even

    further improvement is possible.

    Initial attempts to fabricate this al

    loy by hot swaging have met with

    limited success. It may be necessary to

    break down the cast structure by ex

    trusion before hot swaging to wire.

    Aluminum-Sil icon-Germanium System

    Twelve different compositions were

    formulated and tested for flow tem

    per atu re and flowability-wettability in

    this system. The location of these

    experimental brazing filler metals on

    the ternary layout is shown in Fig. 4.

    Table 4 gives the flow temperatures of

    these alloys along with their composi

    tions. All of the formulated alloys

    melted at reasonable temperatures

    and flowed on the 6061 base metal

    (heavi ly shaded area on the plot) .

    General ly speaking, the flow tempera

    tures of these alloys increased with

    increasing silicon content. All of the

    al loys containing 5% Si (1 , 5 , and 9)

    exhibi ted flow temperatures of 1020F.

    Increasing the silicon content to 20%

    raised the flow temperature to as high

    as 1095F. The lightly shaded area of

    the layout shows those compositions

    which may be of further interest.

    Figure

    11

    shows a series of typical

    pad tests made at different tempera

    tures (in vacuum) with the filler met

    al No. 9. Using successively lower test

    temperatures , we establ ished that the

    flow temperature of this alloy was

    1020 F. Note the excellent flowability

    and wettability of this experimental

    composi t ion at al l temperatures

    tested. We subsequently used this

    same alloy to make the T-joint shown

    in Fig. 12, in which the brazing filler

    metal is preplaced at one end of the

    joint and flow proceeds along the

    capillary. The base metal for the T-

    joint was 6061 and the braze was

    performed by holding for 2.5 minutes

    at 1020F. Good filleting is evident.

    Figure 13 shows a macro of the

    1020F pad tes t performed on al loy

    68-s

    i F E B R U A R Y 1 97 2

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    N o. 5 . The 1020F b raz ing tempera

    ture, 7 minute brazing t ime combina

    tion appears to be slightly excessive

    for this alloy since reaction completely

    through the pad has taken place. Nev

    ertheless, the wetting and flow ex

    hibited is quite good. It should be

    noted that th is brazing temperature is

    lower than that used for commercial

    state-of-the-art brazing filler metals

    and, as such, is a significant advance

    ment in aluminum brazing technol

    ogy.

    Fig ure 14 shows a high magnifica

    tion view of the interface between

    base metal and braze metal for this

    part icular pad tes t . Both photos sug

    gest that this composition is very near

    th e Al-Si-Ge eutect ic composi t ion.

    Figures 15 and 16 show the pad

    test results for one of the higher melt

    ing Al-Si-Ge al loys, No. 8 . This was

    the highest melting of this series of

    alloys. This filler metal also has excel

    lent flow and wetting characteristics

    and is typical of the higher melting

    alloys. The degree of reaction with the

    base metal is satisfactory.

    All of the Al-Si-Ge alloys were

    quite brittle and are not amenable to

    fabrication into wire or sheet by con

    ventional techniques.

    Aluminum-Silicon-Yttrium System

    Twenty different composi t ions were

    formulated and tes ted for f low tem

    pe ra tur e and flowability-wettability in

    this system. The location of these

    experimental brazing filler metals on

    the ternary layout is shown in Fig. 5.

    The l ight ly shaded area shows the

    locat ion of the most promising com

    positions. Table 5 gives the flow tem

    peratures of the al loys that melted

    below the melting point of the 6061

    base metal and the compositions of all

    the alloys tested.

    The higher f low temperatures of

    these alloys rather limit their use per

    se as ternary alloys. However, one

    must remember that addi t ions of mi

    nor quantities of elements such as Cu,

    Sn and Zn could result in considerable

    flow point reduct ion.

    Of the seven experimental composi

    tions in this ternary system which did

    melt below

    1150F,

    excel lent wett ing

    and flow on 6061 base metal was

    obtained. Alloy No. 18 (70 Al- 25 Si-

    5Y)

    exhibited the lowest flow temper

    ature. However, as was the case for

    some compositions in the other series

    investigated, base metal-filler metal in

    teract ion occurred rapidly and exces

    s ive penetrat ion was a problem. Thus,

    careful control of the time-

    temperature thermal cycle (or further

    alloying with additional melting point

    depressants) is necessary.

    The alloys in the

    Al-Si-Y

    system

    were much more fabricable than any

    of the other experimental brazing

    filler metals investigated. They were

    readi ly reduced to V

    16

    -in. wire, as

    shown in Fig. 17.

    Summary an d Conclusion

    During the course of th is program,

    we have developed several brazing

    filler metal compositions that appear

    to exhibit significant improvements

    over exis t ing commercial composi

    t ions. They braze in vacuum at tem

    peratures lower than the flow temper

    atures of commercial brazing al loys

    and have equ al or better flowability.

    F i g . 11Wetting t es t s o n A l - Si -G e N o . 9 m ad e a t s u c c e s s i v e l y h i gh e r t em pe r a t u r e s

    p ro ce e d in g fr o m the le f t . (1) 1020F, (2) 1065F, (3) 1075F, (4) 1095F. Exc e l le n t we t t i n g

    i s e v i d e n t o v e r t h e 75F r a n g e o f t e m p e r a t u r e s ho w n

    ' / '

    ';:::

    V

    :

    :S

    .

    Jr

    F i g . 14Micro

    of i n t e r f ac e be tween 6061

    base m e t a l an d No . 5 A l -S i-Ge a l l o y .

    M a g :

    250X

    F i g . 12T-joint of A l -S i -Ge a l l oy No . 9 an d 6061 base m e t a l .

    B r a z i n g w a s p e r f o r m ed a t 1020F fo r 2 .5 m i n u t e s . E x c e l l e n t

    f l ow i s e v i d e n t

    F i g . 13Macro of p a d t e s t o n A l -S i- Ge a l l o y N o . 5 v a c u u m

    b ra z e d f o r 7 m i n u t e s a t 1022F . A n e x c e s s i v e r e a c t i o n o c c u r r e d

    a t o n e s p o t

    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 | 69 s

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    7/7

    F i g 15Macro of padt e s t on A l -Si -Ge a l l o y No. 8 v a c u u m

    b r a z e d for7 m i n u t e sat1095F

    F i g 17Photoof

    1/16-in.

    w ir e p r o d u c e d bys w a g i n gofAl-Si-Y

    a l loy No. 18 f ro m ac a s t i n g .

    *

    * i

    :

    f

    F i g 16Microo fin t e r f ac e be tween 6061

    b a s e m e t a l and No. 8 Al-S i -Ge a l l oy.

    M a g 250X

    Our lowest flow temperature1020F

    is

    abou t 50F lower than

    the

    gener

    al ly accepted flow temperature of the

    88A1-12

    Si

    comm ercial al loy.

    We specifically studied alloys in

    three ternary systems

    and

    they

    all

    T a b l e 5 - F l o w T e m p e r a t u

    Compositionsof th

    A l l o y

    n u m b e r

    1

    2

    3

    4

    5

    6

    7

    8

    9

    10

    11

    12

    13

    14

    15

    16

    17

    18

    19

    20

    C o m p o s

    Al

    85

    80

    75

    70

    65

    85

    80

    75

    70

    65

    80

    75

    70

    65

    75

    70

    65

    70

    65

    65

    5Al-S

    i t i o n ,

    Si

    5

    5

    5

    5

    5

    10

    10

    10

    10

    10

    15

    15

    15

    15

    20

    20

    20

    25

    25

    30

    r e s a n d

    -Y Alloys

    w t . %

    Y

    10

    15

    20

    25

    30

    5

    10

    15

    20

    25

    5

    10

    15

    20

    5

    10

    15

    5

    10

    5

    F l o w

    t e m p ,

    F

    1120

    1140

    1110

    1130

    1140

    1140

    1095

    flowed on aluminum alloy 6061 in

    vacuum wi thou t

    the use of

    flux.

    The

    Al-Si-ln alloys exhibited flow temper

    atures inthe range 1075to 1095F and

    the Al-Si-Y alloys exhibited flow tem

    pera tu resin therange 1095 to 1140F.

    Alloys

    in the

    Al-Si-Ge system were

    part icularly promising and exhibited

    flow temperatures

    of

    1020

    to

    1095F.

    Of part icular in terest

    in

    this system

    are the 55Al-5S i-40Ge , 45Al-5Si-

    5 0 G e ,

    and

    35Al-5Si-60G e al loys,

    all

    of which flowed at 1020F; these flow

    tempera tu res

    are

    approx imate ly

    50F

    below those

    of

    comm ercial al loys.

    l t should

    be

    emphas ized

    at

    this

    point that wefeel that thefull pote n

    tial

    of

    these alloys

    is yet to be

    rea l

    ized. That is , further work isnecessary

    to show that

    the

    op t imum compos i

    tions

    in

    these systems have been

    found. Secondly, further minor addi

    tions

    of

    other elem ents such as Cu,

    Zn

    and Sn should be investigated since

    they

    may

    result

    in

    further f low tem

    pera tu re reduc t ions and/or wettabili-

    ty-flowability improvemen ts . Also , op

    t imum t ime- temperature relat ionships

    for vacuum brazing with these al loys

    m u s t

    be

    established.

    References

    S c h w a r t z , M. M., Gurtner, F . B., and

    S h u t t , P. K., Jr. , V a c u u m (or F l u x l e s s )

    B r a z i n g - G a s Q u e n c h i n g of 60 6 1 A l u m i n u m

    Alloy, W E L D I N G J O U R N A L , V ol. 46, No. 5,

    May 1 9 67 , pp.

    423-431.

    2B e u y u k i a n ,

    C. S. ,

    F l u x l e s s B r a z i n g

    of

    Ap o l lo C o ld

    PlatesDevelopment

    P r o d u c

    t ion , W E L D I N G J O U R N A L ,

    V ol. 47, No. 9,

    Sep t . 1 9 68 , pp.710-719.

    3 F l u x l e s s B r a z i n g M a k e s H e a d w a y ,

    Iron Age 200 V o l .

    67, No. 8,

    A ug . 10, 1967.

    Unified Theory

    of

    Cumulative Damage

    in

    Metal Fatigue

    B y J u l ie n D u b u c , B u i Q uo c T ha n g , A n d r e B a z e r g u i a n d A n d r e B i r o n

    A rev iew is m a d e of thed i ff e re n t c u m u l a t i v e d a m a g e t h e o r i e s a v a i l a b l e in the

    l i t e r a t u r e . A newa p p r o a c h ( u n i f ie d t h e o ry ) is s u g g e st e d w h i c h can be app l ied

    t o s t r e s s - c o n t ro l l e d

    or

    s t r a i n - c o n t ro l l e d c o n d i t i o n s ,

    an d

    w h i c h c o n s i d e r s

    the

    o rd e r

    o f app l ica t ion

    of

    different s t ress

    or

    s t r a i n l e v e ls . C o m p a r i s o n

    is

    m a d e w i t h

    a

    la rge

    n u m b e r

    of

    test resul ts using sev eral d ifferent le vels .

    The

    t h e o r y

    is

    a l so a pp l ied

    to

    some cases

    of

    r a n d o m l o a d i n g .

    I t

    is

    fo u n d t h a t

    the

    p ro p o s e d t h e o ry y i e l ds

    an

    i m p ro v e d a g re e m e n t w i t h e x p e r i

    men ta l resu l t s , espec ia l ly

    for

    c a s e s w h e re t h e r e

    is a

    la rge d i f fe rence be t we en leve l s .

    Th e p r i c e

    of WRC

    Bulletin

    162 is

    $ 1 . 5 0

    per

    c o p y . O r d e r s

    for ten or

    m o r e

    cop ies shou ld

    be

    s e n t

    to the

    W e l d i n g R e s e a r c h C o u n c i l ,

    3 4 5 E.

    4 7 t h

    St., New

    Y o rk , 1 0 0 1 7 . S in g l e c o p y o rd e r s s h o u l d be sen t to A W S , 2 501 N.W. 7th St.

    M i a m i , F l a . 3 3 1 2 5 .

    W R C

    B u l l e t i n

    N o

    162

    J u n e

    1 9 7 1

    70-s | F E B R U A R Y 1972