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Nonlinear Finite Element Analysis of Concrete Structures

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- 51 -<br />

By use <strong>of</strong> eq. (3) we have then derived the final incremental<br />

equations<br />

deP . d£P llil (3_ €)<br />

J<br />

e<br />

where de is given by eq. (2) and a by eq. (1).<br />

If increasing proportional loading is considered it follows<br />

that<br />

J<br />

where the ratio s. ./a<br />

lj e<br />

that<br />

e<br />

is constant. From this equations follows<br />

^<br />

£P= U £?. ,*.)* (3-6)<br />

\3 13 13/<br />

Eqs. (5) and (6) hold exactly for increasing proportional loading.<br />

It is now assumed that they also apply to nonproportional<br />

loadings. However, while in the finite element program the reinforcement<br />

stresses are not directly determined, the total reinforcement<br />

strains are known as these are assumed to be identical<br />

to the concrete strains. It is therefore advantageous to derive explicitly<br />

the relation between reinforcement stresses and total<br />

strains. Noting that total strains e.. are composed <strong>of</strong> elastic<br />

strains e . . and plastic strains e?. i.e.<br />

e. . = e e . + e?. (3-7)<br />

13 13 13<br />

and working only with principal stresses and strains which is<br />

allowable here inasmuch as the corresponding principal directions<br />

always are assumed to coincide, we therefore write<br />

1 e P<br />

e 1 = - (o x - u(o 2 + o 3 )) + 35- (2 0;L - o 2 - o 3 )<br />

e<br />

e 2 = | (o 2 - u«^ + o 3 )) + fj- (2G 2 - o 1 - o 3 ><br />

e<br />

1 £ P<br />

c 3 = s (o 3 - .j( 0l + o 2 )) + jo - (2o 3 - °1 " a 2><br />

e

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