Issue 29
S. Terravecchia et al., Frattura ed Integrità Strutturale, 29 (2014) 61-73; DOI: 10.3221/IGF-ESIS.29.07
T HE FUNDAMENTAL SOLUTIONS
T
he introduction of eq.(5) in (3a) valid in infinity domain allows to express the latter in terms of displacements only [7,8] and to determine the fundamental solution of the displacements that for 2D solids proves to be
r K
2 2 2 4
I
2
2
r
1
(6)
=
G
uu
16 (1 )
r
2
r
2
[ ] Log r K
r r
2(3 4 )
K
2
0
2
2
r
0 K and
where 2 K are Bessel functions of the second kind and of order 0 and 2, respectively, and r ξ x is the distance between effect ξ and cause x points. One can note that the singularity of the fundamental solution uu G does not depend on r . Indeed, by performing the limit r 0 one obtains 1 ( ) 2(3 4 ) ln(2 ) 1 16 (1 ) uu G ξ x I (7) where is the Eulero constant and the fundamental solution for isotropic gradient elasticity shows singularity of type ln( ) . In eq.(6) the limit of uu G for 0 gives the classic isotropic elasticity solution (Kelvin) with singularity of type ln( ) r .
Table 1 : Fundamental solutions for strain gradient elasticity and relative singularities.
By the fundamental solution uu G in (6), taking in account eqs.(4b,c,d) and using the well-known procedure given in [11], it is possible, by exploiting the known properties of symmetry of the fundamental solutions, to derive the entire tableau provided in Table 1. The fundamental solutions hk G of Tab. 1 are characterized by two subscripts: the first indicates the effect at ξ , i.e. displacement for h u , traction for h t , displacement normal derivative for h g , double traction for h r , corner displacement for C h u , corner force for C h t , stress for h ; whereas the second subscript indicates – through a
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