Design Notes for Various shape

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    The Design Core   Market Assessment 

    Specification

    Concept

    Design

    Detail

    Design

    Manufacture

    Sell 

    DETAIL

    DESIGN

     A vast subject. We will concentrate on:

    Materials Selection

    Process Selection

    Cost Breakdown

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    Materials Selection with Shape

    FUNCTION

    MATERIAL

    PROCESS

    SAPE

    SHAPES FOR TENSION,EN!IN", TORSION,

    #$%&IN"''''''''''''''''''''

    SHAPE FA$TORS''''''''''''''''''''

    PERFOR(AN$E IN!I$ES

    WITH SHAPE

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    Common Modes of Loading 

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    Moments of Sections: Elastic 

    SectionS)a*e A

    +-I 

    +/K 

    +/

    -r π  /

    / r 

    π  /

    - r 

    π 

    -b

    0-

    /b/0/.1   b

    abπ    ba2

    /π 

    + --22

    ba

    ba

    +π 

    bh0-

    2bh

    +

    34.102

    2

    bh

    h

    bhb

    >

       

       −

    -

    /2

    a22-

    /a

    412/a

    rt 

    r r  i o

    π 

    π 

    -

    + --

    t r 

    r r  i o

    2

    // +/π 

    π 

    t r 

    r r  i o

    2

    //

    -

    +-

    π 

    π 

     A 5 $ross'sectional area

    I  5 Secon6 oent o7 area

    ∫ ∫    == tion   y tion y by  Ay I  sec-

    sec

    - 66

    w)ere   y  is easure6 verticall8by  is t)e section wi6t) at y 

    K  5 Resistance to twistin9 o7 section+ Polar oent   o7 a circular section

    ∫ = tion r r   sec 26-π !TLK  θ =w)ere   T  is t)e tor;ue

    L is t)e len9t) o7 t)e s)a7t"  is t)e an9le o7 twist! is t)e s)ear o6ulus

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    Moments of Sections: Elastic 

    bt /

    t ba +   +π 

    bt 

    hhb i o

    -

    +

    +-   bht    +

    +-   bht    +

       

      

     +

    -

    --

    /0

    λ 

    π λ 

      d t 

    t b2

    2

    -

     

     

     

     

      +

    a

    bt a

    20

    /

    2π 

    -<

    +0-

    -

    22

    o

    i o

    bth

    hhb

       

       +

    h

    bt h

    20

    =0 2

    /+=

    -2 bt ht 

    +

    4

    -d t λ 

    /2 0    

      

       −

    b

    t t b

    --

    -

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    Moments of Sections: #ail$re

    SectionS)a*e % +2 &+2

    2

    / r 

    π  2

    - r 

    π 

    =

    2b 2-0.1   b

    ba-

    /π 

    +-

    -

    ba

    ba

    <

    π 

    =

    -bh

    +

    4.02

    --

    bh

    bh

    hb

    >

    +

    2-

    2a

    -1

    2a

    t r 

    r r r 

      i o

    o

    -

    // +/

    π 

    π 

    t r 

    r r r 

      i o

    o

    -

    //

    -

    +-

    π 

    π 

    %  5 Section o6ulusmy 

    I %  =

    w)ere

    y m is t)e noral 6istance 7ro t)e neutral a>isto t)e outer sur7ace o7 t)e bea carr8in9 t)e)i9)est stress

    & 5 Factor in twistin9 siilar to % 

    τ T & =

    w)ere

    τ  is t)e a>iu sur7ace s)ear stress

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    Moments of Sections: #ail$re

    SectionS)a*e % +2 &+2

    t b-

    2

    /-

    - 0-      

       −

    b

    t t b

     

     

     

     

      +a

    bt a 20

    /

    -π 

    +

    +- -

    π 

    ( )

    o

    i o

    o

    bth

    hhh

    b

    − 22=

       

       +

    h

    bt h 20

    2

    -

    tbh-      

       +

    b

    hbt 

    /0

    2

    - -

    /+2

    -2 bt hh

    t + 4+

    2

    -

    hbt 

    +      

       +

    h

    bht 

    /0

    2- -

    /d t λ 

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    Shape #actors: Elastic 

    BENDING

    20

    L

    EI C S' =

    π 

    π 

    //

    -/   Ar I o   ==

    en6in9 sti77ness o7 a bea

    w)ere C 0 is a constant 6e*en6in9 on t)eloa6in9 6etails, L is t)e len9t) o7 t)e bea,

    an6 E  is t)e ?oun9@s o6ulus o7 t)e aterial

    o'o

    'e

    ' I 

    S

    S

    ==φ 

    !e7ine structure 7actor as t)e ratio o7 t)esti77ness o7 t)e s)a*e6 bea to t)at o7 asoli6 circular section wit) t)e sae cross'sectional area t)us:

    -

    / A

    I e'

    π φ   =so,

    TORSION

    L

    K!ST  =Torsional sti77ness o7 a bea

    w)ere L is t)e len9t) o7 t)e s)a7t, ! is t)es)ear (o6ulus o7 t)e aterial.

    π 

    π 

    --

    -/   Ar K o   == -

    - A

    K eT 

    π φ   =so,

    oTo

    T e

    T  K 

    S

    S

    ==φ 

    !e7ine structure 7actor as t)e ratio o7 t)etorsional sti77ness o7 t)e s)a*e6 s)a7t to t)ato7 a soli6 circular section wit) t)e saecross'sectional area t)us:

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    Shape #actors: #ail$re(Strength

    BENDING

    π 

    π 

    //

    -

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    Shape #actors: #ail$re(Strength

    Please Note!

    T)e s)a*e 7actors 7or 7ailure

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    Comparison of Si*e and Shape

    Rectan"#lar sections

    I$sections

    SIDE

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    Shape #actors

    SectionS)a*e Sti77ness Failure

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    Shape #actors cont+d 

    SectionS)a*e Sti77ness Failure

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    Efficiency of Standard Sections

    -

    / A

    I e'

    π φ   =

    ELASTIC BENDING

    S)a*e Factor:

    π 

    φ 

    /lo9lo9-lo9

    e

    ' AI    +=

    Rearran9e 7or I  an6 taCe lo9s:

    Plot lo9I   a9ainst lo9 A  : *arallel lines o7 slo*e -e'φ 

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    Efficiency of Standard Sections

    -

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    Efficiency of Standard Sections

    ELASTIC TORSION

    π 

    φ π φ 

    -lo9lo9-lo9G

    --

    e

    T e

    T    AK  A

    K +==

    TORSIONAL STRENGT

    π 

    φ π φ 

    -lo9lo9

    -2

    lo9G-

    -

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    ,erformance Indices with Shape

    ELASTIC BENDING

    20

    L

    EI C S' =en6in9 sti77ness o7 a bea:

    ELASTIC TORSION

    L

    K!ST  =Torsional sti77ness o7 a s)a7t:

    -

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    ,erformance Indices with Shape

    FAILURE IN BENDING

    f f    % M    σ =Failure w)en oent reac)es:

    FAILURE IN TORSION

    f f    &T    τ =Failure w)en tor;ue reac)es:

     ρ 

    φ σ  2

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    Shape in Materials Selection Maps

    En9ineerin9 Allo8s

    Pol8erFoas

    Woo6s

    En9ineerin9Pol8ers

    Elastoers

    $o*osites

    $eraicsSearc%Re"ion

     A aterial wit) ?oun9@s o6ulus,E  an6 6ensit8, -, wit) a *articular

    section acts as a aterial wit) ane77ective ?oun9@s o6ulus

    an6 6ensit8

    e

    'E E    φ =∗

    e

    'φ  ρ  ρ   =∗

    Per7orance in6e> 7or elasticben6in9 inclu6in9 s)a*e,

    can be written as

     ρ 

    φ  -

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    Shape in Materials Selection Maps

     A aterial wit) stren9t), ) f  an66ensit8, -, wit) a *articular

    section acts as a aterial wit) ane77ective stren9t)

    an6 6ensit8

    -+   f 'f f    φ σ σ    =∗

    -+   f 'φ  ρ  ρ   =∗

    Per7orance in6e> 7or 7ailure inben6in9 inclu6in9 s)a*e,

    can be written as

     ρ 

    σ φ  2

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    Micro/Shape #actors

    (aterial (icro'S)a*e

    K

    (acro'S)a*e, 0

    K

    (acro'S)a*e 7ro(icro'S)a*e6 (aterial,

    10

    5

    #* to now we )ave onl8consi6ere6 t)e role o7acrosco*ic s)a*e on t)e*er7orance o7 7ull8 6ense

    aterials.However, aterials can )aveinternal s)a*e, (icro'S)a*eBw)ic) also a77ects t)eir*er7orance,e.9. cellular soli6s, 7oas,)one8cobs.

    (icro'S)a*e6 (aterial, 1 

    5

    (icro'S)a*e6 (aterial, 1 

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    Micro/Shape #actors

    Pris*atic cells

    Concentric c+lindrical

    s%ells wit% ,oa* )etween

    Fi)res e*)edded

    in a ,oa* *atri-

    $onsi6er a soli6 c8lin6rical bea e>*an6e6, at constantass, to a circular bea wit) internal s)a*e +see ri9)t.

    Sti77ness o7 t)e soli6 bea: 20

    L

    I E C S   oo'o =

    On e>*an6in9 t)e bea, its 6ensit8 7alls 7ro to ,

    an6 its ra6ius increases 7ro to

    o ρ    ρ 

    oo r r 

    -is o7 t)e bea t)en

    T)e sti77ness o7 t)ee>*an6e6 bea is t)us    

     

      

     ==

     ρ 

     ρ oo'

    L

    EI C 

    L

    EI C S

    20

    20

    S%a.e Factor! ρ 

     ρ ψ    o

    o

    e

    'S

    S==

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    Function

    Tie

    ea

    $olun

    S)a7t

    Mats2 Selection: M$ltiple Constraints

    Objective

    (iniu cost

    (iniu wei9)t

    (a>iu store6ener98

    (iniuenvironental

    i*act

    $onstraint

    Sti77ness

    Stren9t)

    Fati9ue

    "eoetr8(ec)anicalT)eralElectricalL..

    In6e>

     ρ 

    -

     ρ 

    σ  2

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    Materials for Safe ,ress$re 3essels

    DESIGN RE/UIREMENTS

    F#nction Pressure vessel 5contain*ressure p

    O)0ecti1e (a>iu sa7et8

    Constraints +a (ust 8iel6 be7ore breaC+b (ust leaC be7ore breaC

    +c Wall t)icCness sall tore6uce ass an6 cost

    ?iel6 be7ore breaC

    -

    -

    ,    

     

     

     

    ≤= f IC 

    C C 

    IC    K 

    C aa

    CK 

    σ π π σ 

    IC K M σ 

    =0

     &eaC be7ore breaC

    IC 

    IC C 

    K  p4 C 

    CK t a

     p4 

    t t 

     p4 

    σ 

    π 

    π σ 

    σ σ 

    --

    /

    -

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    Materials for Safe ,ress$re 3essels

    Searc%Re"ion

    M2 3 '44 MPa

    M' 3 456 *'78

    IC K M σ 

    =0f 

    IC K M σ 

    -

    - =f M    σ =2

    Material   M '9*'78:

    M 29MPa:

    Co**ent

    Tou9) steelsTou9) $u allo8sTou9) Al allo8s

    Ti'allo8sHi9) stren9t) Alallo8s"FRP>> 2>>>

    Hi9) stren9t),but low sa7et8ar9in. "oo67or li9)tvessels.

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    0. E>*ress t)e objective as an e;uation.-. Eliinate t)e 7ree variables usin9 eac) constraint in turn, 9ivin9 a set o7

    *er7orance e;uations +objective 7unctions o7 t)e 7or:

    w)ere f , g  an6 h are e>*ressions containin9t)e 7unctional re;uireents # , 9eoetr8 M 

    an6 aterials in6ices M .

    2. I7 t)e 7irst constraint is t)e ost restrictive +Cnown as t)e acti5e constraint

    t)en t)e *er7orance is 9iven b8 , 0, an6 t)is is a>iie6 b8 seeCin9aterials wit) t)e best values o7 M 0. I7 t)e secon6 constraint is t)e activeone t)en t)e *er7orance is 9iven b8 , - an6 t)is is a>iie6 b8 seeCin9aterials wit) t)e best values o7 M -G an6 so on.

    N.. For a 9iven Function t)e Active $onstraint will be aterial 6e*en6ent.

    M$ltiple Constraints: #ormalised 

    +++

    +++

    +++

    +++

    22222

    -----

    00000

    i i i i i    M h!g # f , 

    M h!g # f , 

    M h!g # f , 

    M h!g # f , 

    ⋅⋅=

    ⋅⋅=

    ⋅⋅=⋅⋅=

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    M$ltiple Constraints: A Simple Analysis

    A LIGT( STIFF( STRONG BEAM T)e object 7unction is   ρ  ALm =

    $onstraint 0: Sti77ness w)ere so,2

    0

    L

    EI C S =

    0-

    /t I  = -

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    M$ltiple Constraints: !raphical 

    lo9 In6e> M 0

       l  o  9 

       I  n   6  e  >     M

       -

    $onstruct a aterials selection a* base6 onPer7orance In6ices instea6 o7 aterials*ro*erties.

    T)e selection a* can be 6ivi6e6 into two6oains in eac) o7 w)ic) one constraint is active.

    T)e $ou*lin9 &ineB se*arates t)e 6oains an6is calculate6 b8 cou*lin9 t)e Objective Functions:

    w)ere C C  is t)e $ou*lin9 $onstantB.

    ------

    00000 ++

    ++M C M 

    !g # f 

    !g # f M  c  ⋅=⋅

    =

    $ou*lin9 &ineM - 5 C C M 0

    M 0 &iite6!oain

    M - &iite6!oain

     A

    (aterials wit) M 6 

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    M$ltiple Constraints: !raphical 

    $ou*lin9 &ineM - 5 C C M 0

    Searc) Area

    $

    lo9 In6e> M 0

       l  o  9 

       I  n   6  e  >

         M   -

    M 0 &iite6!oain

    M - &iite6!oain

     A

    $

    $

     A bo> s)a*e6 Searc) Re9ion is i6enti7ie6 wit) its

    corner on t)e $ou*lin9 &ine.Wit)in t)is Searc) Re9ion t)e *er7orance isa>iie6 w)ilst siultaneousl8 satis78in9 bot)constraints. are 9oo6aterials.

    M 0 &iite6!oain

    M - &iite6!oain

     A

    $ou*lin9 &ineM - 5 C C M 0

    lo9 In6e> M 0

       l  o  9 

       I  n   6  e  >

         M   -

    $

    Searc) Area

     A $

    $)an9in9 t)e 7unctional re;uireents #  or 9eoetr8

    !  c)an9es C C , w)ic) s)i7ts t)e $ou*lin9 &ine, alterst)e Searc) Area, an6 alters t)e sco*e o7 aterialsselection.Now an6 are selectable.

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    8indings for 9igh #ield Magnets

    DESIGN RE/UIREMENTS

    F#nction (a9net win6in9s

    O)0ecti1e (a>iie a9netic 7iel6

    Constraints +a No ec)anical 7ailure+b Te*erature rise Q031$+c Ra6ius r  an6 len9t) L o7

    coil s*eci7ie6

    -r d d 

    L  Turns$urrent i 

    '

    #**er liits on 7iel6 an6 *ulse 6uration areset b8 t)e coil aterial.Fiel6 too )i9) ⇒ t)e coil 7ails ec)anicall8Pulse too lon9 ⇒ t)e coil over)eats

    Classi,ication P#lseD#ration FieldStren"t%

    $ontinuous&on9Stan6ar6S)ort#ltra's)ort

    0 s ' 011 s'0 s01 ' 011 s01 ' 0111 s1.0 ' 01 s

    Q21 T21'=1 T/1'1 T1'41 TM011 T

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    8indings for 9igh #ield Magnets

    ,+7    β α λ  µ 

    L

    i '   f o=T)e 7iel6 +weber

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    8indings for 9igh #ield Magnets

    CONSTRAINT '! O1er%eatin"

    So, 'heat  is a>iie6b8 a>iiin9

    e

     pC M Ω

    =  ρ 

    -

    T)e ener98 o7 t)e *ulse is +4 e 5 avera9e o7 t)e resistance over t)e)eatin9 c8cle, t  p$lse 5 len9t) o7 t)e *ulse causes t)e te*erature o7 t)e coil to rise b8

    w)ere   ?e 5 electrical resistivit8 o7 t)e coil aterialC  p 5 s*eci7ic )eat ca*acit8 o7 t)e coil aterial

     p$lseet 4 i -≈

     ρ  µ   po

     p$lsee

    C d 

    t 'T 

    --

    -Ω

    =∆

    I7 t)e u**er liit 7or t)e c)an9e in te*eratureis UT ma@  an6 t)e 9eoetric constant o7 t)e coilis inclu6e6 t)en t)e secon6 liit on t)e 7iel6 is ,+7 

    ---

    β α  ρ  µ 

     

     

     

     

     

     

    ∆≤

    e p$lse

     po

    heat 

    T C d '

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    8indings for 9igh #ield Magnets

    Material 

    ) y 

    +(Pa

     -

    +(9

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    Searc) Re9ion:#ltra's)ort *ulse

    Searc) Re9ion:lon9 *ulse

    Searc) Re9ion:s)ort *ulse

    HS&A steels

    $u Al'S031.0

    $u'/Sn

    $u'e'$o'Ni

    e'$o**ers

    "P co**ers

    H$ $o**ers

    $u'Nb$u'Al-O2

    $u'Dr 

    8indings for 9igh #ield Magnets

    Material Co**ent

    Contin$o$s and long p$lseHi9) *urit8 co**ersPure Silver 

    Short p$lse$u'Al-O2 co*osites

    H'$ $u'$6 allo8sH'$ $u'Dr allo8sH'$ $u'$r allo8s!rawn $u'Nb co*@s

    ltra short p$lseB$ltra high field $u'e'$o'Ni allo8sHS&A steels

    est c)oice 7or low 7iel6,lon9 *ulse a9nets +)eatliite6

    est c)oice 7or )i9) 7iel6,s)ort *ulse a9nets +)eatan6 stren9t) liite6

    est c)oice 7or )i9) 7iel6,s)ort *ulse a9nets+stren9t) liite6

    e

     pC M Ω

    =  ρ 

    -y M    σ =0