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00694 Pouyan Zarnani - Timber Design Society

00694 Pouyan Zarnani - Timber Design Society

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2.5 EFFECTIVE WOOD THICKNESS<br />

2.5.1 BRITTLE FAILURE<br />

In current tests on LVL and glulam, the average<br />

thickness of the failed block, t block , in the majority of the<br />

brittle failures was observed around 0.85L p . This<br />

thickness corresponds to the elastic deformation of the<br />

rivets since there were no observed plastic deflections.<br />

For brittle failure modes, the effective wood thickness<br />

(Eq. 16) is determined from the elastic deformation of<br />

the rivet modelled as a beam on an elasto-plastic<br />

foundation (Fig. 5). The rivet is supported by springs<br />

with bilinear response that simulate the local nonlinear<br />

embedding behaviour of the timber surrounding it. For<br />

more details regarding the model refer to <strong>Zarnani</strong> and<br />

Quenneville [8].<br />

Rivet<br />

flexural axis<br />

k h<br />

Embedding<br />

stiffness<br />

Figure 5: Spring model of elastic deformation of rivet as<br />

a beam on an elasto-plastic foundation<br />

0.95L p , for L p equals to 28.5 mm<br />

t ef,e ~ 0.85L p , for L p equals to 53.5 mm (16)<br />

0.75L p , for L p equals to 78.5 mm<br />

2.5.2 MIXED FAILURE<br />

Wood effective thickness<br />

w(x)<br />

For some connection groups, considerable decrease of<br />

t block combined to a distortion of rivets was visible. This<br />

failure mode is defined as the mixed mode since the<br />

wood fails with some deflection of the rivets before they<br />

reach complete yielding. In these groups, t block<br />

corresponded to the effective wood thickness, t ef ,<br />

depending on the governing failure mode of the rivets<br />

(Fig. 6).<br />

Mode I m Mode III m Mode IV<br />

Figure 6: Effective thickness based on the rivet<br />

embedded length in different failure modes<br />

x<br />

w<br />

Rotationally fixed<br />

Rivet head<br />

t ef can be derived using Equation 17 based on the<br />

Johansen’s yield theory [9] which is the foundation for<br />

the EYM prediction formulas in Eurocode 5 [5]. The<br />

proposed prediction for the wood strength showed good<br />

agreement with observed values of t block for these groups.<br />

t ef,y =<br />

f h<br />

L p<br />

t ef<br />

2<br />

L p<br />

f<br />

P r<br />

M<br />

f<br />

2<br />

y, l Lp<br />

d<br />

h,0<br />

l<br />

h,0<br />

y,<br />

l<br />

d<br />

l<br />

2<br />

f h<br />

M <br />

L p<br />

t ef<br />

P r<br />

M y<br />

o<br />

P<br />

f h<br />

M y<br />

Mode I m<br />

Mode III m<br />

Mode IV<br />

L p<br />

t ef<br />

P r<br />

(17)<br />

M y<br />

d l is the rivet cross-section dimension bearing on the<br />

wood parallel-to-grain, (equal to 3.2 mm); ƒ h,0 is the<br />

embedment strength of the wood which can be<br />

determined as a function of d l and the density of the<br />

wood [10]; and M y,l is the parallel-to-grain moment<br />

capacity of the rivet, equal to 30000 Nmm [6].<br />

2.6 PROPOSED PROCEDURE<br />

Based on the observation that the effective wood<br />

thickness differs in brittle and mixed failure modes<br />

which affect the wood strength, the following procedure<br />

(Fig. 7) is suggested to determine the load carrying<br />

capacity of the riveted connection for the possible brittle,<br />

ductile and mixed failure modes. In this paper, the rivet<br />

strength and its yielding mode is based on experimental<br />

results which also can be predicted by a consistent yield<br />

model proposed by <strong>Zarnani</strong> and Quenneville [10].<br />

Assume t block = t ef,e corresponding to rivet elastic<br />

deformation to predict wood strength P w<br />

from Eq. 13 and compare with rivet yielding strength P r<br />

If P w < P r<br />

No<br />

If P w ≥ P r<br />

No<br />

P u = P w<br />

(Mixed failure)<br />

Figure 7: Proposed algorithm for different possible brittle,<br />

ductile and mixed failure modes<br />

3 EXPERIMENTAL PROGRAM<br />

3.1 SPECIMENS<br />

Yes<br />

Assume t block =t ef,y corresponding to<br />

rivet yielding mode to predict P w<br />

Yes<br />

Load carrying capacity of<br />

connection P u = P w<br />

(Brittle failure)<br />

P u = P r<br />

(Ductile failure)<br />

The laboratory tests were set up to evaluate the effect of<br />

bottom, edge and end distances on connection strength<br />

and to force and observe the possible connection wood<br />

modes of failure. Specimens were manufactured from<br />

New Zealand Radiata Pine LVL grade 10 and glulam<br />

with grade of 8. The tests series were divided into 26<br />

groups for LVL (Table 1) and 6 groups for glulam<br />

(Table 2). 3 replicates were tested for each group of<br />

specimens for LVL and 4 replicates for glulam. The<br />

parameters for connection geometries (Fig. 4) used<br />

varied from 4 to 8 for N R and N C ; from 15 to 25 mm for<br />

S q and 25 to 50 mm for S p ; L p from 28.5 to 78.5 mm<br />

(with rivet lengths L r of 40, 65 and 90 mm); d z from<br />

0.1X b to 1.1X b ; d e from 0.2X l to 1.9X l and d a from 50 to<br />

125 mm. The specimens had riveted plates on both faces<br />

of timber, making a symmetric connection that better<br />

simulates real applications. The steel side plates were 8.4

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