Introduction to Mechanics of Deformable Solids |
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Page 62
The direction chosen for the shear stress Tns , and therefore the direction of the
force Tn5A , is purely a matter of sign convention and is arbitrary . The choice
made in Fig . 4.16 is the same as in Fig . 4.1 and gives rise to a minus sign in the
...
The direction chosen for the shear stress Tns , and therefore the direction of the
force Tn5A , is purely a matter of sign convention and is arbitrary . The choice
made in Fig . 4.16 is the same as in Fig . 4.1 and gives rise to a minus sign in the
...
Page 240
The force is then multiplied by the cosine ( say , lin ) of the angle between its
direction and the direction of N , to get the component of the force in the direction
of on . An abbreviated notation for Eq . ( 11 . 4 : 7 ) is 3 on = Ě Ě Oijlinlin ( 11 .
The force is then multiplied by the cosine ( say , lin ) of the angle between its
direction and the direction of N , to get the component of the force in the direction
of on . An abbreviated notation for Eq . ( 11 . 4 : 7 ) is 3 on = Ě Ě Oijlinlin ( 11 .
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 – 6 660 = – 400 X 10 – 6 €120 = + 800 x
10 ...
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 – 6 660 = – 400 X 10 – 6 €120 = + 800 x
10 ...
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Bibliographic information
| Title | Introduction to Mechanics of Deformable Solids |
| Author | Daniel Charles Drucker |
| Publisher | McGraw-Hill, 1967 |
| Original from | the University of Michigan |
| Digitized | 29 Nov 2007 |
| Length | 445 pages |
| Export Citation | BiBTeX EndNote RefMan |