SOLUTIONS MANUAL
l
,Table of contents
l l
Partl1:lFoundationslandlelementarylapplications
1. MathematicallPreliminaries
2. Deformation:lDisplacementslandlStrains
3. StresslandlEquilibrium
4. MateriallBehaviorl–lLinearlElasticlSolids
5. FormulationlandlSolutionlStrategies
6. StrainlEnergylandlRelatedlPrinciples
7. Two-DimensionallFormulation
8. Two-DimensionallProblemlSolution
9. Extension,lTorsion,landlFlexureloflElasticlCylinders
Partl2:lAdvancedlapplications
10. ComplexlVariablelMethods
11. AnisotropiclElasticity
12. Thermoelasticity
13. DisplacementlPotentialslandlStresslFunctions:lApplicationsltolThree-DimensionallProblems
14. NonhomogeneouslElasticity
15. Micromechanicsl Applications
16. NumericallFinitelandlBoundarylElementlMethods
,1
1-1.
(a) aiil =la11l +la22l +la33l =l1l+l4l+l1l=l6l (scalar)
aijlaijl =l a11a11l +la12la12l +la13la13l +la21a21l +la22la22l +la23la23l +la31a31l +la32la32l +la33la33
=l1l+l1l+l1l+l0l+l16l+l4l+l0l+l1l+l1l=l25l (scalar)
1 1 11 1 1 1 6 4l
al a =l0 4 20 4 2l =l 0l l 18l l 10l (matrix)
ijl l j
0 1 10 1 1 0 5 3l
k
3l
al bl =lal bl +lal b + al b =l 4 (vector)
ijl l i1l 1 il2l 2 i3l 3 l
j
2
aijlbiblj =la11b1b1l +la12b1b2l +la13b1b3l +la21b2b1l +la22b2b2l +la23b2b3l +la31b3b1l +la32b3b2l +la33b3b3
=l1l+l0l+l2l+l0l+l0l+l0l+l0l+l0l+l4l=l7l (scalar)
b1b1 b1b2 b1b3ll 1 0 2l
blbl =l bl b bl b bl bl =l 0 0 0 (matrix)
2l 3l
il l j l 2 l 1
2l 2
b3b1 b3b2 b3b3l 2 0 4
bibil =lb1b1l +lb2b2l +lb3b3l =l1l+l0l+l4l=l5l (scalar)
(b) aiil =la11l +la22l +la33l =l1l+l2l+l2l=l5l(scalar)
aijlaijl =la11a11l +la12la12l +la13a13l +la21a21l +la22la22l +la23a23l +la31a31l +la32la32l +la33a33
=l1+l4l+l0l+l0l+l4l+1+ l0l+16l+l4l=l30l(scalar)
1 2 01 2 0 1 6 2
al a =l0 2 10 2 1l=l0 8 4l (matrix)
ijl l j
k
0 4 20 4 2 0l 16 8
4
al bl =lal bl +lal bl +lal bl =l3l (vector)
ijl l i1l 1 il2l i3l 3 l
j 2
6
aijbibljl =la11b1b1l+la12b1b2l +la13b1b3l +la21b2b1l +la22b2b2l +la23b2b3l +la31b3b1l +la32b3b2l +la33b3b3
=l4l+l4l+l0l+l0l+l2l+1+ l0l+l4l+l2l=l17l(scalar)
b1b1 b1b2 b1b3ll 4 2 2l
blbl =lbl b bl b bl bl =l 2 1 1 (matrix)
2l 3l
il l j l 2 l 1
2l 2
b3b1 b3b2 b3b3l 2 1 1
bibil =lb1b1l +lb2b2l +lb3b3l =l4l+1+1 l=l6l(scalar)
Copyrightl©l2009,lElsevierlInc.lAlllrightslreserved
.
, 2
(c) aiil =la11l +la22l +la33l =l1l+l0l+l4l=l5l(scalar)
aijlaijl =la11a11l +la12la12l +la13a13l +la21a21l +la22la22l +la23a23l +la31a31l +la32la32l +la33a33
=l1 +1+1+1+ l0l+l4l+l0l+1+16 l=l25l(scalar)
1 1 11 1 1 2 2 7l
al a =l1 0 21 0 2l=l1 3 9ll (matrix)
ijl l j
0 1 40 1 4 1 4l l 18
k
2
al bl =lal bl +lal bl +lal bl =l1l (vector)
ijl l i1l 1 il2l i3l 3 l
j 2
1
aijbibljl =la11b1b1l+la12b1b2l +la13b1b3l +la21b2b1l +la22b2b2l +la23b2b3l +la31b3b1l +la32b3b2l +la33b3b3
=l1 +1+ l0l+1+ l0l+l0l+l0l+l0l+l0l=l3l(scalar)
b1b1 b1b2 b1b3ll 1 1 0l
blbl =lbl b bl b bl bl =l 1 1 0 (matrix)
2l 3l
il l j l 2 l 1
2l 2
b3b1 b3b2 b3b3l 0 0 0
bibil =lb1b1l +lb2b2l +lb3b3l =l1 +1+ l0l=l2l(scalar)
1-2.
1 1
(a) aijl =l (aijl +laljil)l+l (aijl −laljil)
2l 2l
2 1 1 l0 1 1
=l 1 8 3l+l −1 0 1
1l 1l
2l 2l
1 3 2 −1 −1 0
clearlya(ijl)l andl a[ijl]l satisfylthelappropriatelconditions
1l 1l
=l (a + al )l+l (a − al )
(b) aij ij jil
2 ji
2 ij
1l 2 2 0 1l l 0 2 0l
=l 2 4 5l+l −l2 0 −l3
2l 2l
0 5 4 l 0 3 0l
clearlya(ijl)l andl a[ijl]l satisfylthelappropriatelconditions
Copyrightl©l2009,lElsevierlInc.lAlllrightslreserved
.