## Introduction to Mechanics of Deformable Solids |

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Page 98

Therefore , the third

expressed in terms of force , is P - LIN P , L , + a7L70c + ... This

independent

Therefore , the third

**equation**for linear - elastic bars , the deformation conditionexpressed in terms of force , is P - LIN P , L , + a7L70c + ... This

**equation**plus twoindependent

**equations**of equilibrium provides three**equations**for the three ...Page 180

Take the material as homogeneous throughout so that v is constant also , and

use the

1 d ( 0,12 ) ) ( ror ) 2 dr2 dr dor 1 dor 2vor – dr dr d2 20 , v d2 ση le r dr v d2 or vr ...

Take the material as homogeneous throughout so that v is constant also , and

use the

**equation**of equilibrium ( 9.1 : 13 ) to obtain an**equation**in O , alone , v d1 d ( 0,12 ) ) ( ror ) 2 dr2 dr dor 1 dor 2vor – dr dr d2 20 , v d2 ση le r dr v d2 or vr ...

Page 386

The remaining

with the actual di for the compatible set . This time , the equilibrium set should not

cause any displacement unknowns to appear on the left - hand side of the ...

The remaining

**equation**comes from another choice of an equilibrium set , alongwith the actual di for the compatible set . This time , the equilibrium set should not

cause any displacement unknowns to appear on the left - hand side of the ...

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