rincipal stresses o, and o, (o, > 02). The strain energy can be expressed in terms of the strain energy per unit rolume. Then: (a) working from first principles show that the strain energy per unit volume is given by the expression 1 (o}+o}-2va, 2E for a material which follows Hooke's law where E denotes Young's modulus and v denotes Poisson's ratio, and (b) by considering the relations between each of o,, o, Ty respectively and the principal stresses, where x and y are two other mutually perpendicular axes in the same plane, show that the expression 1 [o+o;-2vo,0, + 2(1+ v)r,] 2E

Elements Of Electromagnetics
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Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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11.29 (B/C). A state of two-dimensional plane stress on an element of material can be represented by the
principal stresses o, and o, (o, > 2). The strain energy can be expressed in terms of the strain energy per unit
volume. Then:
(a) working from first principles show that the strain energy per unit volume is given by the expression
1
(o}+o}-2va, o2)
2E
for a material which follows Hooke's law where E denotes Young's modulus and v denotes Poisson's ratio,
and
(b) by considering the relations between each of o,,o,Ty respectively and the principal stresses, where x and y are
two other mutually perpendicular axes in the same plane, show that the expression
1
[o+o-2vo,o, + 2(1+ v)r,]
2E
is identical with the expression given above.
[City U.]
Transcribed Image Text:11.29 (B/C). A state of two-dimensional plane stress on an element of material can be represented by the principal stresses o, and o, (o, > 2). The strain energy can be expressed in terms of the strain energy per unit volume. Then: (a) working from first principles show that the strain energy per unit volume is given by the expression 1 (o}+o}-2va, o2) 2E for a material which follows Hooke's law where E denotes Young's modulus and v denotes Poisson's ratio, and (b) by considering the relations between each of o,,o,Ty respectively and the principal stresses, where x and y are two other mutually perpendicular axes in the same plane, show that the expression 1 [o+o-2vo,o, + 2(1+ v)r,] 2E is identical with the expression given above. [City U.]
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