Civil Engineering Reference
In-Depth Information
a‡a unity, the entire curve corresponds to uncracked sections
(i.e. curve BCD in Figure 10.14 does not exist). The value of a unity
can be found from Eqn 10.19 with e c / e cu =1 and x/h =1 .
v)
It is convenient, and sufficiently accurate, to consider that the
strength capacity of a section is reached (i.e. a = a max in Figure
10.15 ) when the concrete strain reaches e cu simultaneously as the
nth layer of reinforcement yields in compression. The value of a max
can be found from Eqn 10.19 with e c / e cu =1 and x/h =[ x/h ] ycn , where
[ x/h ] ycn is the x/h ratio at which the nth layer of reinforcement yields
in compression (see Eqn 10.26b). When a > a max , the section may be
considered to have crushed; hence equilibrium is not possible and
Eqn 10.23 is not solvable.
10.4.3.3 Solution of Equation 10.23 On a curve for any particular
value of a , if the concrete strain ratio e c / e cu is known at any point, then the
corresponding value of x/h ratio at that point can be found by solving Eqn
10.23. Suppose for the time being, two simplifying assumptions are made:
Assumption (i)
No reinforcement reaches its yield strength, i.e. f si < f yi at all
points on the
curve for the particular value of
a
.
Assumption (ii)
For any positive values assigned to
e cu , Eqn 10.23
is solvable for a real and positive root (i.e. for a real and
positive x/h ).
a
and
e c /
As a result of Assumption (i), r i =1 and m i =0 (see Table 10.1 ) and hence b and
c become constant. Suppose the concrete strain ratio e c / e cu at a certain point on
a curve for a given value of a is known, then the corresponding x/h ratio
at the point can be determined from Eqn 10.23 as follows:
Case 1:
e c / e cu £ [ e c / e cu ] x/h =1
Reference to Figure 10.14 makes it clear that the point lies to the
left of B; that is x/h 1 and the section is uncracked . Hence, in Eqn
10.24a, the limit of integration e Ó c is itself a function of x/h (see
Section 10.4.2.3). Therefore, in Eqn 10.23 the coefficient a is a
function of x/h; the solution of Eqn 10.23 requires an iterative
method, say the bisection method (Conte and Boor, 1980).
Case 2:
e c / e cu >[ e c / e cu ] x/h =1
The point now lies to the right of B in Figure 10.14; that is x/h <1
and the section is cracked . Hence, in Eqn 10.24a, e Ó c =0 (see
Figure 10.11 b). Eqn 10.23 is therefore a quadratic equation, the
roots of which are
(10.25)
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