Introduction to Mechanics of Deformable Solids |
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Page 5
4 Problems 197 chapter 10 Combined loading , superposition 199 chapter 11
Principal stresses and principal strains . Stress and strain as tensors 218 10 . 1
Superposition of Solutions 199 10 . 2 Problems 205 10 . 3 The Thin - walled
Circular ...
4 Problems 197 chapter 10 Combined loading , superposition 199 chapter 11
Principal stresses and principal strains . Stress and strain as tensors 218 10 . 1
Superposition of Solutions 199 10 . 2 Problems 205 10 . 3 The Thin - walled
Circular ...
Page 250
26 Plane strain . Principal strains ta , e given . and ( see Eq . ( 11 . 4 : 1 ) ] the
change in volume per unit volume 61 + 62 + 63 = €z + ty tez ( 11 . 6 : 9 ) If the
material is incompressible , Ez + Ey + € , = 0 and the strain tensor is a strain -
deviation ...
26 Plane strain . Principal strains ta , e given . and ( see Eq . ( 11 . 4 : 1 ) ] the
change in volume per unit volume 61 + 62 + 63 = €z + ty tez ( 11 . 6 : 9 ) If the
material is incompressible , Ez + Ey + € , = 0 and the strain tensor is a strain -
deviation ...
Page 259
A . Principal strains in the surface and their orientation B . en in the surface at 60°
and at 120° to the axial direction 11 . 19 An equiangular rosette gives the
following strain readings : 60 = 100 X 10 – 6 €60 = - 400 x 10 - 6 €120 = + 800 x
10 - 6 ...
A . Principal strains in the surface and their orientation B . en in the surface at 60°
and at 120° to the axial direction 11 . 19 An equiangular rosette gives the
following strain readings : 60 = 100 X 10 – 6 €60 = - 400 x 10 - 6 €120 = + 800 x
10 - 6 ...
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