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Support CenterVerification examplesFillet weld in lap joint
Fillet weld in lap joint
SteelConnection designVerificationsEN (Eurocode)Welds

Fillet weld in lap joint

This article is also available in
ENCZDEESFRITPTNLHUROKRPLTHTRVIZH

This article is a selected chapter from the book Component-based finite element design of steel connections by Prof. Wald et al. The chapter is focused on the verification of welds. This chapter was slightly modified for this web, and the results were updated.

Description

The objective of this chapter is the verification of the component-based finite element method (CBFEM) of a fillet weld in a lap joint with the component method (CM). Two plates are connected in three configurations, namely with a transverse weld, with a longitudinal weld, and a combination of transverse and longitudinal welds. The length and throat thickness of the weld are the varying parameters in the study. The study also covers long welds whose resistance is reduced due to stress concentration. The joint is loaded by a normal force.

Analytical model

The fillet weld is the only component examined in the study. The welds are designed to be the weakest component in the joint. The weld is designed according to EN 1993-1-8:2005. The design resistance of the fillet weld is determined using the Directional method given in Cl. 4.5.3.2 in ENย 1993-1-8:2005. The available calculation methods for checking the strength of fillet welds are based upon the simplifying assumption that stresses are uniformly distributed within a throat section of a fillet weld, leading to the normal stresses and shear stresses shown in Fig. 4.1.1, as follows:

  • ฯƒโŠฅ is the normal stress perpendicular to the throat section;
  • ฯƒโˆฅ is the normal stress parallel to the axis of the weld in its cross-section;
  • ฯ„โŠฅ is the shear stress (in the plane of the throat section) perpendicular to the axis of the weld;
  • ฯ„โˆฅ is the shear stress (in the plane of the throat section) parallel to the axis of the weld.

The normal stress ฯƒโˆฅ parallel to the axis is not considered when verifying the design resistance of a weld.

Fig.ย 4.1.1ย Stressesย inย aย throatย sectionย ofย aย filletย weld\textsf{\textit{\footnotesize{Fig. 4.1.1 Stresses in a throat section of a fillet weld}}}Fig.ย 4.1.1ย Stressesย inย aย throatย sectionย ofย aย filletย weld

The design resistance of the fillet weld will be sufficient if the following are both satisfied:

ฯƒโŠฅ2+3โ‹…(ฯ„โŠฅ2+ฯ„โŠฅ2)โ‰คfuฮฒwฮณM2\sqrt{\sigma_{\perp}^2 + 3 \cdot ( \tau_{\perp}^2 + \tau_{\perp}^2 )} \le \frac{f_\textrm{u}}{\beta_\textrm{w} \gamma_\textrm{M2}}ฯƒโŠฅ2โ€‹+3โ‹…(ฯ„โŠฅ2โ€‹+ฯ„โŠฅ2โ€‹)โ€‹โ‰คฮฒwโ€‹ฮณM2โ€‹fuโ€‹โ€‹

ฯƒโŠฅโ‰ค0.9fuฮณM2\sigma_{\perp} \le \frac{0.9 f_\textrm{u}}{\gamma_\textrm{M2}}ฯƒโŠฅโ€‹โ‰คฮณM2โ€‹0.9fuโ€‹โ€‹

In lap joints longer than 150โ‹…a150 \cdot a150โ‹…a, the reduction factor ฮฒLw,1\beta_{\mathrm{Lw,1}}ฮฒLw,1โ€‹ is given by:

ฮฒLw,1=1.2โˆ’0.2Lj150a\beta_{\mathrm{Lw,1}} = 1.2 - \frac{0.2 L_\textrm{j}}{150 a}ฮฒLw,1โ€‹=1.2โˆ’150a0.2Ljโ€‹โ€‹ย ย but ย ย ฮฒLw,1โ‰ค1.0\beta_{\mathrm{Lw,1}} \le 1.0ฮฒLw,1โ€‹โ‰ค1.0

Numerical model

The weld component in CBFEM is described in General theoretical background and EN theoretical background. Nonlinear elastic-plastic material is used for welds in this study. The limiting plastic strain is reached in the longer part of the weld, and stress peaks are redistributed.

Verification of resistance

An overview of the considered examples and the material properties is provided in Tab. 4.1.1. The weld configurations are T for transverse, P for parallel weld, and TP for a combination of both; see the geometry in Fig. 4.1.2. The steel grade was S235 (fy = 235 MPa, fu = 360 MPa, E = 210 GPa, ฮฒw = 0,8). Partial safety factors were ฮณM0 = 1.0, ฮณM2 = 1.25. The geometry of the model is shown in Fig. 4.1.2. The plates have a thickness of 20 mm. The connection is symmetrical, and the plate is pulled out of the welded splice connection. The length and width of the plates are adjusted according to the length of the parallel and transverse weld. The weld resistance is always the governing failure mode. The weld throat thickness is 3 mm. The lengths of the transverse and parallel welds vary in this parametric study.

Drawingย 4.1ย Jointย geometryย withย dimensions\textsf{\textit{\footnotesize{Drawing 4.1 Joint geometry with dimensions}}}Drawingย 4.1ย Jointย geometryย withย dimensions

Design weld resistance calculated by CBFEM is compared with the results of CM. The results are presented in Tab. 4.1.1 โ€“ 4.1.3 and Fig. 4.1.3 โ€“ 4.1.5.

Fig.ย 4.1.2ย Specimenย geometry\textsf{\textit{\footnotesize{Fig. 4.1.2 Specimen geometry}}}Fig.ย 4.1.2ย Specimenย geometry

Transverse welds resistance calculationย 

ฯƒโŠฅ2+3โ‹…(ฯ„โŠฅ2+ฯ„โˆฅ2)โ‰คfuฮฒwโ‹…ฮณM2\sqrt{ \sigma_{\perp}^2 + 3 \cdot \left( \tau_{\perp}^2 + \tau_{\parallel}^2\right)} \leq \frac{f_\textrm{u}}{\beta_{\textrm{w}} \cdot \gamma_{\textrm{M2}}}ฯƒโŠฅ2โ€‹+3โ‹…(ฯ„โŠฅ2โ€‹+ฯ„โˆฅ2โ€‹)โ€‹โ‰คฮฒwโ€‹โ‹…ฮณM2โ€‹fuโ€‹โ€‹

ฯƒโŠฅ=ฯ„โŠฅ=ฯƒN2=NLtโ‹…aโ‹…12\sigma_{\perp} = \tau_{\perp} = \frac{\sigma_\textrm{N}}{\sqrt{2}} = \frac{N}{L_{\textrm{t}} \cdot a}\cdot \frac{1}{\sqrt{2}}ฯƒโŠฅโ€‹=ฯ„โŠฅโ€‹=2โ€‹ฯƒNโ€‹โ€‹=Ltโ€‹โ‹…aNโ€‹โ‹…2โ€‹1โ€‹

ฯ„โˆฅ=0\tau_{\parallel} = 0ฯ„โˆฅโ€‹=0

(ฯƒN2)2+3โ‹…(ฯƒN2)2โ‰คfuฮฒwโ‹…ฮณM2\sqrt{ \left( \frac{\sigma_\textrm{N}}{\sqrt{2}} \right)^2 + 3 \cdot \left( \frac{\sigma_\textrm{N}}{\sqrt{2}} \right)^2} \leq \frac{f_\textrm{u}}{\beta_{\textrm{w}} \cdot \gamma_{\textrm{M2}}}(2โ€‹ฯƒNโ€‹โ€‹)2+3โ‹…(2โ€‹ฯƒNโ€‹โ€‹)2โ€‹โ‰คฮฒwโ€‹โ‹…ฮณM2โ€‹fuโ€‹โ€‹

(NLtโ‹…aโ‹…12)2+3โ‹…(NLtโ‹…aโ‹…12)2โ‰คfuฮฒwโ‹…ฮณM2\sqrt{ \left( \frac{N}{L_{\textrm{t}}\cdot a}\cdot \frac{1}{\sqrt{2}} \right)^2 + 3 \cdot \left( \frac{N}{L_{\textrm{t}}\cdot a}\cdot \frac{1}{\sqrt{2}} \right)^2} \leq \frac{f_\textrm{u}}{\beta_{\textrm{w}} \cdot \gamma_{\textrm{M2}}}(Ltโ€‹โ‹…aNโ€‹โ‹…2โ€‹1โ€‹)2+3โ‹…(Ltโ€‹โ‹…aNโ€‹โ‹…2โ€‹1โ€‹)2โ€‹โ‰คฮฒwโ€‹โ‹…ฮณM2โ€‹fuโ€‹โ€‹

Nโ‰คfuโ‹…Ltโ‹…aฮฒwย โ‹…ย ฮณM2ย โ‹…ย 2N \leq \frac{f_\textrm{u} \cdot L_{\textrm{t}}\cdot a }{\beta_{\textrm{w}} ย \cdot ย \gamma_{\textrm{M2}} ย \cdot ย \sqrt{2}}Nโ‰คฮฒwโ€‹ย โ‹…ย ฮณM2โ€‹ย โ‹…ย 2โ€‹fuโ€‹โ‹…Ltโ€‹โ‹…aโ€‹

ฯƒโŠฅ=NLtโ‹…aโ‹…12โ‰คfuย โ‹…ย 0.9ฮณM2\sigma_{\perp}= \frac{N}{L_{\textrm{t}} \cdot a}\cdot \frac{1}{\sqrt{2}} \leq \frac{f_\textrm{u} ย \cdot ย 0.9}{ \gamma_{\textrm{M2}}}ฯƒโŠฅโ€‹=Ltโ€‹โ‹…aNโ€‹โ‹…2โ€‹1โ€‹โ‰คฮณM2โ€‹fuโ€‹ย โ‹…ย 0.9โ€‹

Nโ‰คfuย โ‹…Ltโ‹…ย aย โ‹…ย 0.9ย โ‹…ย 2ฮณM2N \leq \frac{f_{u} ย \cdot L_{\textrm{t}}\cdot ย a ย \cdot ย 0.9 ย \cdot ย \sqrt{2}}{ \gamma_{\textrm{M2}} }Nโ‰คฮณM2โ€‹fuโ€‹ย โ‹…Ltโ€‹โ‹…ย aย โ‹…ย 0.9ย โ‹…ย 2โ€‹โ€‹

Where:

aaa - weld throat thickness

NNN - the normal force acting on the beam

LtL_{\textrm{t}}Ltโ€‹ - total transverse weld lengthย 

ฮฒw\beta_{\mathrm{w}}ฮฒwโ€‹ - correlation factor taken from EN 1993-1-8 Table 4.1

fuf_\textrm{u}fuโ€‹ - nominal ultimate tensile strength of the weaker part joined

ฮณM2\gamma_{\mathrm{M2}}ฮณM2โ€‹ - partial safety factor for welds

Parallel weld resistance calculation

ฯƒโŠฅ2+3โ‹…(ฯ„โŠฅ2+ฯ„โˆฅ2)โ‰คfuฮฒwโ‹…ฮณM2\sqrt{ \sigma_{\perp}^2 + 3 \cdot \left( \tau_{\perp}^2 + \tau_{\parallel}^2\right)} \leq \frac{f_\textrm{u}}{\beta_{\mathrm{w}} \cdot \gamma_{\mathrm{M2}}}ฯƒโŠฅ2โ€‹+3โ‹…(ฯ„โŠฅ2โ€‹+ฯ„โˆฅ2โ€‹)โ€‹โ‰คฮฒwโ€‹โ‹…ฮณM2โ€‹fuโ€‹โ€‹

ฯƒโŠฅ=ฯ„โŠฅ=0\sigma_{\perp} = \tau_{\perp} = 0ฯƒโŠฅโ€‹=ฯ„โŠฅโ€‹=0

ฯ„โˆฅ=VLpย โ‹…ย a\tau_{\parallel} = \frac{V}{L_{\textrm{p}} ย \cdot ย a}ฯ„โˆฅโ€‹=Lpโ€‹ย โ‹…ย aVโ€‹

ย 3โ‹…(ฯ„โˆฅ)2โ‰คfuฮฒwโ‹…ฮณM2\sqrt{ ย 3 \cdot \left( \tau_{\parallel} \right)^2} \leq \frac{f_\textrm{u}}{\beta_{\mathrm{w}} \cdot \gamma_{\mathrm{M2}}}ย 3โ‹…(ฯ„โˆฅโ€‹)2โ€‹โ‰คฮฒwโ€‹โ‹…ฮณM2โ€‹fuโ€‹โ€‹

ย 3โ‹…(ย VLpโ‹…a)2โ‰คfuฮฒwโ‹…ฮณM2\sqrt{ ย 3 \cdot \left( ย \frac{V}{L_{\textrm{p}} \cdot a}\right)^2} \leq \frac{f_\textrm{u}}{\beta_{\mathrm{w}} \cdot \gamma_{\mathrm{M2}}}ย 3โ‹…(ย Lpโ€‹โ‹…aVโ€‹)2โ€‹โ‰คฮฒwโ€‹โ‹…ฮณM2โ€‹fuโ€‹โ€‹

V=fuย โ‹…ย Lpโ‹…ย aย โ‹…ย ฮฒLw1ฮฒwย โ‹…ย ฮณM2ย โ‹…ย 3V = \frac{f_\textrm{u} ย \cdot ย L_{\textrm{p}} \cdot ย a ย \cdot ย \beta_{\mathrm{Lw1}}}{\beta_{\mathrm{w}} ย \cdot ย \gamma_{\mathrm{M2}} ย \cdot ย \sqrt{3}}V=ฮฒwโ€‹ย โ‹…ย ฮณM2โ€‹ย โ‹…ย 3โ€‹fuโ€‹ย โ‹…ย Lpโ€‹โ‹…ย aย โ‹…ย ฮฒLw1โ€‹โ€‹

Where:

aaa - weld throat thickness

VVV - shear force acting on beam

LtL_{\textrm{t}}Ltโ€‹ - total parallel welds length

ฮฒw\beta_{\mathrm{w}}ฮฒwโ€‹ - correlation factor taken from EN 1993-1-8 Table 4.1

ฮฒLw1\beta_{\mathrm{Lw1}}ฮฒLw1โ€‹ - long weld reduction factor, EN 1993-1-8 Equation 4.9

fuf_\textrm{u}fuโ€‹ - nominal ultimate tensile strength of the weaker part joined

ฮณM2\gamma_{\mathrm{M2}}ฮณM2โ€‹ - partial safety factor for welds

Transverse and parallel calculationย 

The resistance calculated by hand for a transverse and parallel weld combination is simply the sum of the transverse and parallel resistances derived from the equations above.ย 

Results Presentation

Tab.ย 4.1.1ย Parallelย weldsย results\textsf{\textit{\footnotesize{Tab. 4.1.1 Parallel welds results}}}Tab.ย 4.1.1ย Parallelย weldsย results

Fig.ย 4.1.3ย Comparisonย ofย loadย resistancesย ofย parallelย welds\textsf{\textit{\footnotesize{Fig. 4.1.3 Comparison of load resistances of parallel welds}}}Fig.ย 4.1.3ย Comparisonย ofย loadย resistancesย ofย parallelย welds

Fig.ย 4.1.3.aย Influenceย ofย weldย lengthย onย resistance\textsf{\textit{\footnotesize{Fig. 4.1.3.a Influence of weld length on resistance}}}Fig.ย 4.1.3.aย Influenceย ofย weldย lengthย onย resistance

Tab.ย 4.1.2ย Transverseย welds\textsf{\textit{\footnotesize{Tab. 4.1.2 Transverse welds}}}Tab.ย 4.1.2ย Transverseย welds

Fig.ย 4.1.4ย Comparisonย ofย loadย resistancesย ofย transverseย welds\textsf{\textit{\footnotesize{Fig. 4.1.4 Comparison of load resistances of transverse welds}}}Fig.ย 4.1.4ย Comparisonย ofย loadย resistancesย ofย transverseย welds

Fig.ย 4.1.4.aย Influenceย ofย weldย lengthย onย resistance\textsf{\textit{\footnotesize{Fig. 4.1.4.a Influence of weld length on resistance}}}Fig.ย 4.1.4.aย Influenceย ofย weldย lengthย onย resistance

Tab.ย 4.1.3ย Groupedย welds\textsf{\textit{\footnotesize{Tab. 4.1.3 Grouped welds}}}Tab.ย 4.1.3ย Groupedย welds

Fig.ย 4.1.5ย Comparisonย ofย loadย resistancesย ofย group\textsf{\textit{\footnotesize{Fig. 4.1.5 Comparison of load resistances of group}}}Fig.ย 4.1.5ย Comparisonย ofย loadย resistancesย ofย group

The resistance of parallel welds, transverse welds, and multi-oriented weld groups is nearly identical according to CM and CBFEM. The biggest difference in this study is 6% in load resistance.

The CBFEM results of parallel welds are slightly conservative but start to diverge for long welds. The reduction of resistance due to long welds is not captured by CBFEM, but it is not expected that welds longer than 200ร—throat thickness could appear in any connection, and up to this length, the results are still very close.

For transverse welds, CBFEM provides very consistent results with 2โ€“4% higher resistance.

Benchmark example

Inputs

Member 1 โ€“ Iw60x500

โ€ข Welded from plates with thickness t = 20 mm

โ€ข Width b = 500 mm

โ€ข Web is removed by Opening manufacturing operation

โ€ข Steel S235

Member 2 โ€“ Plate 20x1000

โ€ข Thickness t = 20 mm

โ€ข Width b = 1000 mm

โ€ข Steel S235

โ€ข Offset ex = โ€“90 mm

Transverse fillet weld at both sides of Member 2

โ€ข Throat thickness a = 3 mm

โ€ข Weld length Lt = 100 mm

Parallel fillet weld at both sides of Member 2

โ€ข Throat thickness a = 3 mm

โ€ข Weld length Lp = 100 mm

Output

โ€ข Design resistance in tension FRd = 387 kN (It should be noted that the resistance was calculated using the "Stop at limit strain" function. Consequently, the actual CBFEM resistance may be marginally higher.)

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