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Nonlinear Finite Element Analysis of Concrete Structures

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- 113 -<br />

600 ^<br />

500 t-<br />

CT uit = 518 MPa<br />

400 -<br />

'o<br />

| 300 ~<br />

200 l<br />

100 -<br />

0 *<br />

o<br />

Peter (1964) "<br />

approximation<br />

..... a... I<br />

4 5<br />

Fig. 5.1-2: Experimental and approximated stressstrain<br />

curve for bar material.<br />

perimental values and for the predicted values using different<br />

K-values. It should be recalled that for a = 10° and 20°the experimental<br />

panels include vertical reinforcement not considered<br />

in the analysis. It is also important to note that the loading<br />

causes cracks so large that aggregate interlock can hardly be<br />

present, i.e., all forces along the crack planes must be attributed<br />

to the reinforcement bars. As an illustration, the largest<br />

horizontal displacement occurs experimentally for a = 30°. Experimentally<br />

the mean crack width was determined to be 0.44 mm<br />

and assuming that all horizontal displacements occurred along<br />

the crack planes the maximum mean horizontal displacement along<br />

a crack plane was determined to be 0.11 mm which is quite small<br />

compared to the crack width.<br />

From the horizontal displacements shown in fig. 3 it appears<br />

that an optimal value <strong>of</strong> K seems to be located in the range<br />

K = 0.10-0.25. However, fig. 4 indicates that the predicted vertical<br />

displacements are strongly dependent also on the K-value.<br />

This constitutes in fact a major objection against the method<br />

used here for considering the lateral stiffness <strong>of</strong> a reinforcement<br />

bar, as in reality the axial and lateral stiffnesses <strong>of</strong> a<br />

bar are quite independent. Obviously, the axial bar stiffness is<br />

the matter <strong>of</strong> major importance and even small K-values between

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