Issue 33

Y. Wang et alii, Frattura ed Integrità Strutturale, 33 (2015) 345-356; DOI: 10.3221/IGF-ESIS.33.38

After determining the direction of the maximum variance, the shear strain resolved along this direction, MV ( ) t  , can directly be evaluated, at any instant, t , of the load history, through the following relationship:

1 2

1 2 1 2

       

       

x ε (t )

(t )

(t )

xy

xz

x     y        n n n

  t

1 2

 

  

MV

(14)

q q q

γ (t ) ε (t )

yz γ (t )

xy

y

x

y

z

2

xz 1 1 γ (t ) γ (t ) ε (t ) 2 2 yz z

z

      t t t     q q q

Var

)(

        

        

 , ,

n n n

n n    n

n n    n

    

    

    

    

1

Var

)(

 , ,

k

1

n n n

Var

)(

 

1

 , ,

n n n

Figure 2 : Flowchart summarizing the algorithm for the determination of the critical plane orientation.

, and the stress normal to the plane experiencing

The shear stress resolved along the maximum variance direction, MV ( ) t 

, can be evaluated, at any instant, t , of the load history, through the

the maximum variance of resolved shear strain, n ( ) t 

following relationships:

    

x       y          z n n n

x 

 

(t ) (t ) (t )

(t ) (t ) (t )

(t ) (t ) (t )

xy

xz

  t

 

 

 

y 

q q q

(15)

x

y

z

MV

xy

yz

z 

xz

yz

349

Made with FlippingBook - professional solution for displaying marketing and sales documents online