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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 EN 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:

  • σ⊥ is the normal stress perpendicular to the throat section;
  • σ∥ is the normal stress parallel to the axis of the weld in its cross-section;
  • τ⊥ is the shear stress (in the plane of the throat section) perpendicular to the axis of the weld;
  • τ∥ is the shear stress (in the plane of the throat section) parallel to the axis of the weld.

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

Fig. 4.1.1 Stresses in a throat section of a fillet weld\textsf{\textit{\footnotesize{Fig. 4.1.1 Stresses in a throat section of a fillet weld}}}Fig. 4.1.1 Stresses in a throat section of a fillet weld

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

σ⊥2+3⋅(τ⊥2+τ⊥2)≤fuβwγM2\sqrt{\sigma_{\perp}^2 + 3 \cdot ( \tau_{\perp}^2 + \tau_{\perp}^2 )} \le \frac{f_\textrm{u}}{\beta_\textrm{w} \gamma_\textrm{M2}}σ⊥2​+3⋅(τ⊥2​+τ⊥2​)​≤βw​γM2​fu​​

σ⊥≤0.9fuγM2\sigma_{\perp} \le \frac{0.9 f_\textrm{u}}{\gamma_\textrm{M2}}σ⊥​≤γM2​0.9fu​​

In lap joints longer than 150⋅a150 \cdot a150⋅a, the reduction factor βLw,1\beta_{\mathrm{Lw,1}}βLw,1​ is given by:

βLw,1=1.2−0.2Lj150a\beta_{\mathrm{Lw,1}} = 1.2 - \frac{0.2 L_\textrm{j}}{150 a}βLw,1​=1.2−150a0.2Lj​​  but   βLw,1≤1.0\beta_{\mathrm{Lw,1}} \le 1.0βLw,1​≤1.0

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, βw = 0,8). Partial safety factors were γM0 = 1.0, γM2 = 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.

Drawing 4.1 Joint geometry with dimensions\textsf{\textit{\footnotesize{Drawing 4.1 Joint geometry with dimensions}}}Drawing 4.1 Joint geometry with dimensions

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

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

Transverse welds resistance calculation 

σ⊥2+3⋅(τ⊥2+τ∥2)≤fuβw⋅γM2\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}}}σ⊥2​+3⋅(τ⊥2​+τ∥2​)​≤βw​⋅γM2​fu​​

σ⊥=τ⊥=σN2=NLt⋅a⋅12\sigma_{\perp} = \tau_{\perp} = \frac{\sigma_\textrm{N}}{\sqrt{2}} = \frac{N}{L_{\textrm{t}} \cdot a}\cdot \frac{1}{\sqrt{2}}σ⊥​=τ⊥​=2​σN​​=Lt​⋅aN​⋅2​1​

τ∥=0\tau_{\parallel} = 0τ∥​=0

(σN2)2+3⋅(σN2)2≤fuβw⋅γM2\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}}}(2​σN​​)2+3⋅(2​σN​​)2​≤βw​⋅γM2​fu​​

(NLt⋅a⋅12)2+3⋅(NLt⋅a⋅12)2≤fuβw⋅γM2\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}}}(Lt​⋅aN​⋅2​1​)2+3⋅(Lt​⋅aN​⋅2​1​)2​≤βw​⋅γM2​fu​​

N≤fu⋅Lt⋅aβw ⋅ γM2 ⋅ 2N \leq \frac{f_\textrm{u} \cdot L_{\textrm{t}}\cdot a }{\beta_{\textrm{w}}  \cdot  \gamma_{\textrm{M2}}  \cdot  \sqrt{2}}N≤βw​ ⋅ γM2​ ⋅ 2​fu​⋅Lt​⋅a​

σ⊥=NLt⋅a⋅12≤fu ⋅ 0.9γM2\sigma_{\perp}= \frac{N}{L_{\textrm{t}} \cdot a}\cdot \frac{1}{\sqrt{2}} \leq \frac{f_\textrm{u}  \cdot  0.9}{ \gamma_{\textrm{M2}}}σ⊥​=Lt​⋅aN​⋅2​1​≤γM2​fu​ ⋅ 0.9​

N≤fu ⋅Lt⋅ a ⋅ 0.9 ⋅ 2γM2N \leq \frac{f_{u}  \cdot L_{\textrm{t}}\cdot  a  \cdot  0.9  \cdot  \sqrt{2}}{ \gamma_{\textrm{M2}} }N≤γM2​fu​ ⋅Lt​⋅ a ⋅ 0.9 ⋅ 2​​

Where:

aaa - weld throat thickness

NNN - the normal force acting on the beam

LtL_{\textrm{t}}Lt​ - total transverse weld length 

βw\beta_{\mathrm{w}}βw​ - correlation factor taken from EN 1993-1-8 Table 4.1

fuf_\textrm{u}fu​ - nominal ultimate tensile strength of the weaker part joined

γM2\gamma_{\mathrm{M2}}γM2​ - partial safety factor for welds

Parallel weld resistance calculation

σ⊥2+3⋅(τ⊥2+τ∥2)≤fuβw⋅γM2\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}}}σ⊥2​+3⋅(τ⊥2​+τ∥2​)​≤βw​⋅γM2​fu​​

σ⊥=τ⊥=0\sigma_{\perp} = \tau_{\perp} = 0σ⊥​=τ⊥​=0

τ∥=VLp ⋅ a\tau_{\parallel} = \frac{V}{L_{\textrm{p}}  \cdot  a}τ∥​=Lp​ ⋅ aV​

 3⋅(τ∥)2≤fuβw⋅γM2\sqrt{  3 \cdot \left( \tau_{\parallel} \right)^2} \leq \frac{f_\textrm{u}}{\beta_{\mathrm{w}} \cdot \gamma_{\mathrm{M2}}} 3⋅(τ∥​)2​≤βw​⋅γM2​fu​​

 3⋅( VLp⋅a)2≤fuβw⋅γM2\sqrt{  3 \cdot \left(  \frac{V}{L_{\textrm{p}} \cdot a}\right)^2} \leq \frac{f_\textrm{u}}{\beta_{\mathrm{w}} \cdot \gamma_{\mathrm{M2}}} 3⋅( Lp​⋅aV​)2​≤βw​⋅γM2​fu​​

V=fu ⋅ Lp⋅ a ⋅ βLw1βw ⋅ γM2 ⋅ 3V = \frac{f_\textrm{u}  \cdot  L_{\textrm{p}} \cdot  a  \cdot  \beta_{\mathrm{Lw1}}}{\beta_{\mathrm{w}}  \cdot  \gamma_{\mathrm{M2}}  \cdot  \sqrt{3}}V=βw​ ⋅ γM2​ ⋅ 3​fu​ ⋅ Lp​⋅ a ⋅ βLw1​​

Where:

aaa - weld throat thickness

VVV - shear force acting on beam

LtL_{\textrm{t}}Lt​ - total parallel welds length

βw\beta_{\mathrm{w}}βw​ - correlation factor taken from EN 1993-1-8 Table 4.1

βLw1\beta_{\mathrm{Lw1}}βLw1​ - long weld reduction factor, EN 1993-1-8 Equation 4.9

fuf_\textrm{u}fu​ - nominal ultimate tensile strength of the weaker part joined

γM2\gamma_{\mathrm{M2}}γM2​ - partial safety factor for welds

Transverse and parallel calculation 

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. 

Results Presentation

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

Fig. 4.1.3 Comparison of load resistances of parallel welds\textsf{\textit{\footnotesize{Fig. 4.1.3 Comparison of load resistances of parallel welds}}}Fig. 4.1.3 Comparison of load resistances of parallel welds

Fig. 4.1.3.a Influence of weld length on resistance\textsf{\textit{\footnotesize{Fig. 4.1.3.a Influence of weld length on resistance}}}Fig. 4.1.3.a Influence of weld length on resistance

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

Fig. 4.1.4 Comparison of load resistances of transverse welds\textsf{\textit{\footnotesize{Fig. 4.1.4 Comparison of load resistances of transverse welds}}}Fig. 4.1.4 Comparison of load resistances of transverse welds

Fig. 4.1.4.a Influence of weld length on resistance\textsf{\textit{\footnotesize{Fig. 4.1.4.a Influence of weld length on resistance}}}Fig. 4.1.4.a Influence of weld length on resistance

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

Fig. 4.1.5 Comparison of load resistances of group\textsf{\textit{\footnotesize{Fig. 4.1.5 Comparison of load resistances of group}}}Fig. 4.1.5 Comparison of load resistances of 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 200×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 2–4% higher resistance.

Benchmark example

Inputs

Member 1 – Iw60x500

• Welded from plates with thickness t = 20 mm

• Width b = 500 mm

• Web is removed by Opening manufacturing operation

• Steel S235

Member 2 – Plate 20x1000

• Thickness t = 20 mm

• Width b = 1000 mm

• Steel S235

• Offset ex = –90 mm

Transverse fillet weld at both sides of Member 2

• Throat thickness a = 3 mm

• Weld length Lt = 100 mm

Parallel fillet weld at both sides of Member 2

• Throat thickness a = 3 mm

• Weld length Lp = 100 mm

Output

• 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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