## Introduction to Mechanics of Deformable Solids |

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Page 120

10 Creep and recovery in nonlinear Maxwell assemblage of five

Sketch drawn for n large in M + M ; " = 0 19 of 2 times the stress in the inner bars .

The larger the value of n , the closer the ratio comes to unity . Therefore , when n

is ...

10 Creep and recovery in nonlinear Maxwell assemblage of five

**equal**bars .Sketch drawn for n large in M + M ; " = 0 19 of 2 times the stress in the inner bars .

The larger the value of n , the closer the ratio comes to unity . Therefore , when n

is ...

Page 187

1 : 39 ) for the outer shell 2 , where 2tı = 2t2 = b – a if both shells are taken to be

of

243 00 + po From ( 9 . 1 : 37 ) : P12 = paino = 2426 60 + potom From ( 9 .

1 : 39 ) for the outer shell 2 , where 2tı = 2t2 = b – a if both shells are taken to be

of

**equal**thickness . From ( 9 . 1 : 39 ) : ( 9 . 1 : 40 ) 62 2t 6 62 ( 9 . 1 : 41 ) P21 =243 00 + po From ( 9 . 1 : 37 ) : P12 = paino = 2426 60 + potom From ( 9 .

Page 380

the imagined disk must stretch by u * sin 2a . No other internal work is done , and

the tensile forces obviously do positive work because of the elongation . Just as ...

**Equal**and opposite tensile forces P act on the disk . In the motion from H to H " ,the imagined disk must stretch by u * sin 2a . No other internal work is done , and

the tensile forces obviously do positive work because of the elongation . Just as ...

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