ABSTRACT

Hypothesis:”e two materials are in principle bonded together. More precisely, we make the following assumptions:

◾ Both matrix m and ber f have the same longitudinal strain value noted εℓ. ◾ ”ere is afreedom along zon the interface between the two materials, allowing distinct

values of normal strain in each of the two materials:

ε εz m

”e state of stress resulting from an applied force F can therefore be written as

∑→ 

  

  

∑ → 

  

  

σ σ 0 0 0 0 0

0 0 0

0 0

0 0 0

0 0 0

and the corresponding state of strain as

∑ ∑ m

→ 

  

  

→ 

  

  

ε ε

ε

ε ε

ε

0 0

0 0

0 0

0 0

0 0

0 0

Eachmaterialbeingassumedlinearlyelasticandisotropic,itsbehaviorlaw(so-calledHooke’s law), is written in the form

∑ = + ∑− ∑( ) ( )1 v

E v E

trace I (10.1)

inwhichΣrepresentsthestraintensor,Σthestresstensor,andI theunitarytensor.E andvare the elastic constants of the considered material.