## Introduction to Mechanics of Deformable Solids |

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Page 76

Po po . P + PO Fig . 5 . 3

proper treatment of thick spherical shells must be postponed to Chap . 9 .

However , it is worth noting here that rather thick shells of ductile metal , ts / r

perhaps as high ...

Po po . P + PO Fig . 5 . 3

**Addition**of hydrostatic pressure po to Fig . 5 . 2 . Aproper treatment of thick spherical shells must be postponed to Chap . 9 .

However , it is worth noting here that rather thick shells of ductile metal , ts / r

perhaps as high ...

Page 77

to zero ( Fig . 5 . 4 ) and results in a uniaxial compression po = 0 in the radial

direction . This uniaxial compression o is equivalent to ( produces the same

creep ...

**Addition**of this hydrostatic pressure reduces the biaxial tensile stress in the shellto zero ( Fig . 5 . 4 ) and results in a uniaxial compression po = 0 in the radial

direction . This uniaxial compression o is equivalent to ( produces the same

creep ...

Page 296

Note that in Eq . ( 13 . 2 : 4 ) the presence of the shear - stress component Tae in

n > 1 increases the magnitude of ċa " and éc " over their values for ga , o alone .

Note that in Eq . ( 13 . 2 : 4 ) the presence of the shear - stress component Tae in

**addition**to the normal - stress components Oa , Oc increases J , and therefore forn > 1 increases the magnitude of ċa " and éc " over their values for ga , o alone .

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