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 o2 (o, >). 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 2E

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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 o2 (o, > 02). 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
(o}+o-2vo, o)
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, tyy respectively and the principal stresses, where x and yare
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 o2 (o, > 02). 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 (o}+o-2vo, o) 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, tyy respectively and the principal stresses, where x and yare 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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