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Building Design and Construction Handbook - Merritt - Ventech!

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5.42 SECTION FIVE<br />

not appreciably greater than the average for the web section alone, if it is assumed<br />

that the flanges take no shear.<br />

5.5.14 Combined Shear <strong>and</strong> Bending Stress<br />

For deep beams on short spans <strong>and</strong> beams made of low-strength materials, it is<br />

sometimes necessary to determine the maximum stress ƒ� on an inclined plane<br />

caused by a combination of shear <strong>and</strong> bending stress—v <strong>and</strong> ƒ, respectively. This<br />

stress ƒ�, which may be either tension or compression, is greater than the normal<br />

stress. Its value may be obtained by application of Mohr’s circle (Art. 5.3.6), as<br />

indicated in Fig. 5.10, but with ƒ y � 0, <strong>and</strong> is<br />

5.5.15 Beam Deflections<br />

�<br />

��<br />

2<br />

ƒ ƒ 2<br />

ƒ� � � v � (5.60)<br />

2 2<br />

When a beam is loaded, it deflects. The new position of its longitudinal centroidal<br />

axis is called the elastic curve.<br />

At any point of the elastic curve, the radius of curvature is given by<br />

EI<br />

R � (5.61)<br />

M<br />

where M � bending moment at the point<br />

E � modulus of elasticity<br />

I � moment of inertia of the cross section about the neutral axis<br />

Since the slope dy/dx of the curve is small, its square may be neglected, so that,<br />

for all practical purposes, 1/R may be taken equal to d 2 y/dx 2 , where y is the<br />

deflection of a point on the curve at a distance x from the origin of coordinates.<br />

Hence, Eq. (5.61) may be rewritten<br />

2 dy<br />

M � EI (5.62)<br />

2 dx<br />

To obtain the slope <strong>and</strong> deflection of a beam, this equation may be integrated, with<br />

M expressed as a function of x. Constants introduced during the integration must<br />

be evaluated in terms of known points <strong>and</strong> slopes of the elastic curve.<br />

Equation (5.62), in turn, may be rewritten after one integration as<br />

B M<br />

� � � � � dx (5.63)<br />

B A<br />

A EI<br />

in which � A <strong>and</strong> � B are the slopes of the elastic curve at any two points A <strong>and</strong> B.<br />

If the slope is zero at one of the points, the integral in Eq. (5.63) gives the slope<br />

of the elastic curve at the other. It should be noted that the integral represents the<br />

area of the bending-moment diagram between A <strong>and</strong> B with each ordinate divided<br />

by EI.

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