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Formability test set-up

Formability test set-up

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This paper presents results of experimental studies of forming limit curves (FLC) for sheet forming under complex strain paths. The Nakazima-type formability tests have been performed for the as-received steel blank and for the blank pre-strained by13%. Prestraining leads to abrupt change of strain path in the blank deformation influencing the form...

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... formability tests consisting in stretching of the blank over a hemispherical punch have been carried out for the steel grade DC04 1 mm thick. Figure 1 shows the geometry and set-up of the tools. The tests have been per- formed for the as-received sheet supplied by the manufacturer and for the blank pre-stretched in uniaxial tension conditions by13% along the rolling direction. ...
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... this way point C p in polar coordinates is obtained. Applying this procedure to a number of points defining the FLC in the Cartesian coordinates ( Fig. 9(a)) we can obtain the FLC in the polar coordinates ( Fig. 9(b)). Transformation of the FLC for the complex strain paths is explained in Fig. 10. The transformation procedure is modified by taking the angle defining the strain path at the last stage before fracture as the polar coordinate θ and accumulative evaluation of the equivalent plastic ...
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... FLCs for different pre-strain coincide with good accuracy in the polar coordinates. This allowed them to take a certain average curve in the polar coordinates as the strain-path independent FLC. Now, the transformation procedure from the Cartesian to the polar coordinates will be applied to the set of our own experimental FLCs presented in Fig. 11. The set includes the as-received FLC and two FLCs for different pre-strains. The FLCs considered are also presented in Fig. 8. One of the FLCs in Fig. 11 have been obtained by swapping coordinates in one of the FLCs presented in Fig. 8. Applying the transformation described earlier a set of FLCs in the polar coordinates shown in Fig. ...
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... as the strain-path independent FLC. Now, the transformation procedure from the Cartesian to the polar coordinates will be applied to the set of our own experimental FLCs presented in Fig. 11. The set includes the as-received FLC and two FLCs for different pre-strains. The FLCs considered are also presented in Fig. 8. One of the FLCs in Fig. 11 have been obtained by swapping coordinates in one of the FLCs presented in Fig. 8. Applying the transformation described earlier a set of FLCs in the polar coordinates shown in Fig. 12 is obtained. Keeping the angle constant and av- eraging the radius in the polar diagrams an average FLC is obtained which can be used as the strain-path ...
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... in Fig. 11. The set includes the as-received FLC and two FLCs for different pre-strains. The FLCs considered are also presented in Fig. 8. One of the FLCs in Fig. 11 have been obtained by swapping coordinates in one of the FLCs presented in Fig. 8. Applying the transformation described earlier a set of FLCs in the polar coordinates shown in Fig. 12 is obtained. Keeping the angle constant and av- eraging the radius in the polar diagrams an average FLC is obtained which can be used as the strain-path in dependent FLC. Analysing the set of transformed FLCs in the polar co- ordinates ( Fig. 12) we observed a larger discrepancy than we expected. However, such discrepancy can be ...
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... Fig. 8. Applying the transformation described earlier a set of FLCs in the polar coordinates shown in Fig. 12 is obtained. Keeping the angle constant and av- eraging the radius in the polar diagrams an average FLC is obtained which can be used as the strain-path in dependent FLC. Analysing the set of transformed FLCs in the polar co- ordinates ( Fig. 12) we observed a larger discrepancy than we expected. However, such discrepancy can be understood since similar disagreement can be noticed for some cases in [21]. This motivated us to check an alternative transformation to the polar coordinates. Instead of the equivalent plastic strain we propose to take the absolute value of the ...
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... such discrepancy can be understood since similar disagreement can be noticed for some cases in [21]. This motivated us to check an alternative transformation to the polar coordinates. Instead of the equivalent plastic strain we propose to take the absolute value of the thickness strain |ε 3 | obtained from the condition of constant volume as Fig. 12. Set of FLCs after transformation to the polar coordinates according to [21,20] ...
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... idea is consistent with the shift of the FLC along the line of constant thickness proposed by Hosford and Caddell in [10], which was discussed above. Applying this transformation to the set of the FLCs shown in Fig. 11 we obtain the polar FLCs plotted in Fig. 13. Much better coincidence of the transformed FLCs can be seen in comparison with the polar FLCs shown in Fig. 12. This indicates that the new concept of the polar FLCs is worth further studies and ...
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... idea is consistent with the shift of the FLC along the line of constant thickness proposed by Hosford and Caddell in [10], which was discussed above. Applying this transformation to the set of the FLCs shown in Fig. 11 we obtain the polar FLCs plotted in Fig. 13. Much better coincidence of the transformed FLCs can be seen in comparison with the polar FLCs shown in Fig. 12. This indicates that the new concept of the polar FLCs is worth further studies and ...
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... with the shift of the FLC along the line of constant thickness proposed by Hosford and Caddell in [10], which was discussed above. Applying this transformation to the set of the FLCs shown in Fig. 11 we obtain the polar FLCs plotted in Fig. 13. Much better coincidence of the transformed FLCs can be seen in comparison with the polar FLCs shown in Fig. 12. This indicates that the new concept of the polar FLCs is worth further studies and ...

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... However, in complex forming processes where the loading path characteristic is nonlinear, the FLD cannot accurately predict the formability of sheet metals [3]. The polar effective plastic strain-forming limit diagram (PEPS-FLD) is one of the forming limit diagrams that has been applied to estimate the formability of sheet metal forming in place of the conventional FLC [4]. Because the PEPS-FLD has a number of advantages, like not being susceptible to history of deformation and being independent of hardening law selection [5], having no significant/noticeable path dependency, independence with the stress-strain relation, and a similar shape to the conventional FLC [6], the transformation of the FLD to the PEPS diagram can be done without much difficulty using the assumption of proportional loading for each source point selected on the FLC [7]. ...
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... The uniformity of strain in the centre region is not related to fracture of the specimen but it defines the quality of biaxial testing. (3) The third equation [23] allows to compare all samples taking into account both previously introduced factors: FR and COV. This equation is called the Cost Function (CF) and it uses wf coefficient which indicates, which of the first two coefficients is more important. ...
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... Most of industrial sheet metal forming processes involves the existence of complex non-linear strain paths during the manufacturing operations, making the conventional FLC unsuitable tool for assessing formability (Graf and Hosford, 1993;Barata-Rocha et al., 1985;Rojek et al., 2013). To overcome this limitation, the proposal of pathindependent forming limit curves has been intensively evaluated in the research community. ...
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