Laminate Thickness and Vf

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    Fibre Volume Fraction and

    Laminate Thickness

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    How much fibre…?

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    How much reinforcement?

    Weight fraction Used in manufacture.

    May refer to fibre or resin - !"# manufacturers will

    s$ecify a glass content of %e.&.' () wt*+ a $re$re&su$$lier mi&ht &i,e a resin content of wt*.

    Volume fraction 

    Used in desi&n to calculate com$osite $ro$erties. /lmost always refers to fibre content.

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    0ei&ht fraction ↔ ,olume fraction

    con,ersion

    V   W 

    W W f 

    f f 

    f f f m

    =+ −

    1

    1 % ' 1

     ρ 

     ρ ρ 2

    For the s$ecial case of a two-com$onent

    com$osite %e& fibre and matri3'4

    W   V 

    V V f 

    f f 

    f f m f  

    =+ −

     ρ 

     ρ ρ   % '2

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    Volume fraction - weight fraction conversion(epoxy resin matrix)

    5

    5.(

    5.

    5.6

    5.7

    2

    5 5.( 5. 5.6 5.7 2

    fibre weight fraction

       f   i   b

      r  e  v  o   l  u  m  e   f  r  a  c   t

       i  o  n

    &lass

    H8 carbon

    aramid

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    Ma3imum fibre ,olume fraction

    Theoretically9 a unidirectional fibre com$osite could ha,e Vf  :;5*.

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    Ma3imum fibre ,olume fraction

    For other forms of reinforcement9 ma3imum ,olume fraction also de$ends

    on the detailed arran&ement of the fibres.

    The followin& ,alues are ty$ical4

      stitched >non-crim$ 5.6  wo,en fabric 5. - 5.))

      random

    %cho$$ed strand mat' 5.2) - 5.()

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    How much fibre?

    @ommercial reinforcements are characterised by

    their areal weight (Aw  ).  This is sim$ly the wei&ht

    %usually &i,en in &' of 2 m( of the reinforcement. /w 

    de$ends on many factors - fibre density9 tow orbundle siAe9 wea,e style9 etc.

     /w may ran&e from )5 &1m( or less %for li&htwei&ht

    surfacin& tissues'9 u$ to more than (555 &1m( for

    some hea,ywei&ht non-crim$ fabrics.

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    Laminate thickness

    fibre

    matri3

    hi&h matri3 content

    low fibre content

    B thick laminate

    low matri3 content

    hi&h fibre content

    B thin laminate

    Two laminates9 both containin& ) $lies of reinforcement4

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    Laminate thickness

    Fibre ,olume fraction is thus in,ersely $ro$ortionalto laminate thickness.

    nAV 

    f  ρ 

    =

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    Ply thickness vs fibre volume fraction (glass)

    5

    5.)

    2

    2.)

    (

    (.)

    5.2 5.( 5. 5. 5.) 5.6 5.=

    fibre volume fraction

      p   l  y   t   h   i  c   k  n  e  s  s   (  m  m   )

    (55 &1m(

    55 &1m(

    )5 &1m(

    655 &1m(

     Area weight 

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    Ply thickness vs fibre volume fraction (HS carbon)

    5

    5.(

    5.

    5.6

    5.7

    2

    2.(

    2.

    2.6

    5.( 5. 5. 5.) 5.6 5.= 5.7

    fibre volume fraction

      p   l  y   t   h   i  c   k  n  e  s  s   (  m  m   )

    255 &1m(

    2)5 &1m(

    (55 &1m(

    55 &1m(

    )55 &1m(

     Area weight 

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    Example calculationsExample calculations

    !! 0hat will be the thickness of a laminate

    consistin& of ( layers of )5 &1m( cho$$ed

    strand mat if a resin to &lass ratio %by wei&ht'of (42 is used?

    "!"!  0hat fibre ,olume fraction is achie,ed if(

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    "ules of Mi3ture

    for Clastic #ro$erties

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    "ules of Mi3tures are mathematical

    e3$ressions which &i,e some $ro$erty ofthe com$osite in terms of the $ro$erties9

    Duantity and arran&ement of its

    constituents.

    They may be based on a number of

    sim$lifyin& assum$tions9 and their use indesi&n should tem$ered with e3treme

    cautionE

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    ensity

    For the s$ecial case of a fibre-reinforced matri34

    mmf f    VV   ρ+ρ=ρ

    since V f  + V m = 2

    mf f f    'V2%V   ρ−+ρ=ρ

    mmf f    '%V   ρ+ρ−ρ=ρ

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    "ule of mi3tures density for

    &lass1e$o3y com$osites

    5

    )55

    2555

    2)55

    (555

    ()55

    555

    5 5.( 5. 5.6 5.7 2

    fibre volume fraction

         k    g     #    m     $

    ρf 

    ρm

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    Micromechanical models for stiffness

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    Unidirectional $ly - lon&itudinal

    tensile modulus

    E 1 = E f  V f  + E m ( 1-V f )

    Gote the similarity to the rules of mi3ture

    e3$ression for density.

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    This rule of

    mi3tures is a&ood fit to

    e3$erimental

    data

    %source4 Hull9

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    !eneralised rule of mi3tures for

    tensile modulus

    E = L o E f  V f  + E m (1-V f )

    η L is a len&th correction factor. Ty$ically9 η L ≈ 2

    for fibres lon&er than about 25 mm.

    η o corrects for non-unidirectional reinforcement4

    η o

    unidirectional 2.5bia3ial 5.)bia3ial at ±)o 5.()random %in-$lane' 5.=)random %F' 5.(

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    %ule of mixtures tensile mo&ulus

    (glass fibre#polyester)

    5

    25

    (5

    55

    )5

    65

    5 5.( 5. 5.6 5.7

    fibre volume fraction

       t  e  n  s   i   l  e  m  o   &  u   l  u  s

       (   '   P  a   )

    UF

    bia3ial

    @8M

    %ule of mixtures tensile mo&ulus

    ($ carbon fibre)

    5

    )5

    255

    2)5

    (55

    5 5.( 5. 5.6 5.7

    fibre volume fraction

       t  e  n  s   i   l  e  m  o   &  u   l  u  s   (   '   P  a   )

    UF

    bia3ial

    Duasi-isotro$ic

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