Introduction to Mechanics of Deformable Solids |
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Page 233
15a , if oz > Oy , the direction of o , in the absence of would be the direction of the
heavy arrow 07 . The plane on which o would act would be given by the heavy
vertical line . If , alone were present , o , = 0y = 0 , the direction of o1 would be the
...
15a , if oz > Oy , the direction of o , in the absence of would be the direction of the
heavy arrow 07 . The plane on which o would act would be given by the heavy
vertical line . If , alone were present , o , = 0y = 0 , the direction of o1 would be 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 3 on = { 2 rijlinlin ( 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 3 on = { 2 rijlinlin ( 11 .
Page 370
23 , the shear stresses Tay and Tz . are in the directions indicated by the arrows .
The magnitude of the shear flow ... The direction of V , V = P , will vary with
material behavior but certainly cannot be vertical . Therefore the direction of P
cannot ...
23 , the shear stresses Tay and Tz . are in the directions indicated by the arrows .
The magnitude of the shear flow ... The direction of V , V = P , will vary with
material behavior but certainly cannot be vertical . Therefore the direction of P
cannot ...
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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 California |
| Digitized | 11 Mar 2008 |
| Length | 445 pages |
| Export Citation | BiBTeX EndNote RefMan |