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Biomedical Engineering – From Theory to Applications

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Orthopaedic Modular Implants Based on Shape Memory Alloys<br />

The matrix of eigenvec<strong>to</strong>rs is:<br />

X 1/ 3 1/<br />

6 1/ 2 0 0 0<br />

<br />

1/ 3 1/ 6 1/<br />

2 0 0 0<br />

<br />

1/ 3 2/ 6 0 0 0 0<br />

0 0 0 1 0 0<br />

<br />

0 0 0 0 1 0<br />

<br />

0 0 0 0 0 1<br />

b. In the case of monoclinic crystallographic structure:<br />

The eigenvalues are:<br />

S 1<br />

λ =<br />

<br />

C +C + C +C +4C<br />

<br />

C C C 0 0 C <br />

11<br />

<br />

<br />

C12 C13 12<br />

C22 C23 13<br />

C23 C33 0<br />

0<br />

0<br />

0<br />

16<br />

C<br />

<br />

26 <br />

C 36<br />

0 0 0 C44 C45 0 <br />

<br />

0 0 0 C C 0 <br />

45 55<br />

<br />

C16 C26 C36 0 0 C66<br />

<br />

2 2<br />

4 44 55 44 55 45<br />

2 <br />

; 2 2<br />

λ 5= C 44+C55-C 44+C 55 +4C45<br />

2<br />

and λ 1,λ 2,λ 3,λ4are the roots of the equation:<br />

455<br />

(13)<br />

(14)<br />

1 <br />

<br />

(15)<br />

4 3 2<br />

λ -I1λ +I2λ-I3λ+I 4=0<br />

(16)<br />

where Ik is the sum of the diagonal minors of k degree obtained by cutting the fourth and<br />

the fifth columns and rows in matrix [S].<br />

c. In the case of orthorhombic crystallographic structure:<br />

The eigenvalues are:<br />

S and λ 1,λ 2,λ3are the roots of the equation:<br />

C11 C12 C13 0 0 0 <br />

<br />

C12 C22 C23 0 0 0<br />

<br />

<br />

C13 C23 C33 0 0 0 <br />

<br />

0 0 0 C44 0 0 <br />

0 0 0 0 C55 0 <br />

<br />

0 0 0 0 0 C <br />

66 <br />

(17)<br />

λ 4=C 44;<br />

λ 5=C 55;<br />

λ 6=C 66<br />

(18)<br />

3 ' 2 ' '<br />

λ -I1λ +I2λ-I 3=0<br />

(19)

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