Crack Paths 2012
numerical analyses on different S F R Cstructural elements, able to account for both
material non-linearity and fibre resistant contribution in the post-cracking stage.
At each loading increment (or iteration within a fixed increment) and for each single
element in which the structure is subdivided, the total strain vector {8} calculated from
the adopted FE code is passed to the user-material subroutine. Following the above
described procedure, these strain values are used for the evaluation of the proper
material stiffness matrix depending on the current cracking stage and, knownit, for the
determination of corresponding stresses, which are then passed back to the FE code for
the execution of external convergence checks. O n this point, it should be reminded that
the proposed model is based on a strain decomposition scheme in the cracked stage; as a
consequence, it is also necessary to check the convergence on total strain through an
internal iterative procedure, like the one summarizedin the fl o wchart reported Fig. 3.
for the k-th external iteration andthe j-th internal one
{scij : {Sop-1’ {scrlij : {sik' {grail-4
%
u
I
{at —> [0.11 {as = {elk —> 11x11
4 [D11 : ( (113,104+ (113M104 )‘1 ( [I] + (113.101 [13.11)
{ 8 c r l }_j )W l j :V1‘i — >[])crl]‘i
l1 {6s}j : lDslj {elk {6P : lDlj {$}k—> { iscij =_ {6P I’ isslj
I’ {EJJ ([Dcl Jil. isclj
I
{6W1}J : {6}]
_’ {SHIP =([Dcr1]J)_1 {6M1}J
{ 8 P: {8c}j+ { S u l p
l
{e}j I {Elk
N O
e11 Eras“ ; isms" Ewe?"
[1 YES
[D] k I [D]
{gik I {6}J
Figure 3. Flow chart of the internal iterative procedure to obtain strain decomposition.
C O M P A R I SWO IN TS EH X P E R I M E NRTEASLU L T S
S F R Cbeamsin bending
In order to verify the effectiveness of the proposed procedure, an experimental program
carried out on S F R Cbeams in bending has been first considered [8]. More in details,
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