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F. K. Kong MA, MSc, PhD, CEng, FICE, FIStructE, R. H. Evans CBE, DSc, D ès Sc, DTech, PhD, CEng, FICE, FIMechE, FIStructE (auth.)-Reinforced and Prestressed Concrete-Springer US (1987)

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176 Reinforced concrete beams-the serviceability limit states

where x is measured from B.

Comments

The above results were first given the name curvature-area theorems in

the first edition of the book, published in 1975; a formal proof using the

principle of virtual work was given subsequently [16).

For estimating the deflections of concrete structures, the curvature-area

theorems have distinct advantages over the conventional moment-area

theorems:

(a) Unlike the moment-area theorems, the curvature-area theorems

express the purely geometrical relations between the slopes, 0, the

deflections Ll and the curvatures 1/r. Since the relations are purely

geometrical, their validity is independent of the mechanical properties

of the materials. That is, the curvature-area theorems are

equally applicable irrespective of whether the structure is elastic or

plastic or elasto-plastic.

(b) Unlike the moment-area theorems, the curvature-area theorems

can be used even where the deformations are caused by other effects

than bending moments, e.g. by shrinkage and creep. Once the

curvatures are known, the slopes and deflections are completely

defined by the curvature-area theorems; whether the curvatures

have been caused by bending moments or by shrinkage and creep

does not affect the results.

Example 5.5-1

Figure 5.5-1 shows the curvature diagrams for a beam of uniform flexural

rigidity El, acted on by various loadings. Determine the midspan

deflection a in each case.

SOLUTION

(a) Referring to the curvature diagram for beam (a),

shaded area = ! (1) (1..) = 1 (1..)

2 2 rm 4 rm

Moment of shaded area about left support

= £(,:)(~) = f~(,:)

From the curvature-area theorem, this is the deflection of the left

support from the tangent at midspan, and is numerically equal to the

midspan deflection a. Therefore

a = 12z2(t)

(b) Similarly,

a= (~~,:)ell) = ii 2 (t)

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