Issue 52

M. Fouzia et alii, Frattura ed Integrità Strutturale, 52 (2020) 281-298; DOI: 10.3221/IGF-ESIS.52.22

By noting (

) moy

l 

being the mean shear stress deformation of the adhesive,

the mean shear displacement of the

A moy

A

adhesive,

A G the adhesive shear modulus and φ the diameter of the fixations, we have:

(

)

(

)

2

=

bL n −

 

A f

/

/ 4

(4)

moy

and

) ( A

)

) ( A

)

(

(

2

2

=

bL n −

 

=

bL n −

 

=

f

/ 4

G

/ 4

A moy

A moy

(5)

(

) ( /

)

(

)

2

=

e bL n −

 

( G l

/ 4

A

moy A

The authors considering that the bolts are deformed only by shearing at the joint plane. Noting G B the shear modulus if the bolt, T B the uniform stress of the bolt and Δ l B the shear deformation of the bolt we have:

2

B B f =



/ ( ( n

) / 4)

(6)

and

(

)

2



n

B

(

)

2

=

= 



(7)

f

l

/

en

/ 4

B

moy

B

4

by noting:

( ) l 

) B

=

k

(8)

(

l

moy

A

we obtain:

(

)

(

) 2

(

)

=

G k l 

e n 

(9)

f

)/

/ 4

B B

moy

A

Thus:

(

)

(

)

(

)

(

)

 

 

2

2

( =  l

e G bL n −



+



(10)

f

1/

/ 4

kG n

/ 4

moy

A

B

A

By defining α as the tress concentration factor expressed by:

(

)

/ total l  =   l

(11)

moy

A

and considering

(

)

/ =  = A total G l e

(12)

G

max

A moy A

A

where ( τ max ) A is the maximum stress at the adhesive, we obtain :

(

)

(

)

(

)

 

 

2

2

=

e G bL n  −



+



(13)

f

1/

/ 4

kG n

/ 4

l

A

B

total

286

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