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Building Design and Construction Handbook - Merritt - Ventech!

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FIGURE 5.25 Unit stresses on a beam cross<br />

section caused by bending of the beam.<br />

5.5.11 Moment of Inertia<br />

STRUCTURAL THEORY 5.39<br />

ƒI<br />

M � (5.54)<br />

C<br />

M is the bending moment at the section,<br />

ƒ is the normal unit stress in a plane at<br />

a distance c from the neutral axis (Fig.<br />

5.25), <strong>and</strong> I is the moment of inertia of<br />

the cross section with respect to the neutral<br />

axis. If ƒ is given in pounds per<br />

square inch (psi), I in in 4 , <strong>and</strong> c in<br />

inches, then M will be in inch-pounds.<br />

For maximum unit stress, c is the distance<br />

to the outermost fiber. See also<br />

Arts. 5.5.11 <strong>and</strong> 5.5.12.<br />

The neutral axis in a symmetrical beam is coincidental with the centroidal axis;<br />

i.e., at any section the neutral axis is so located that<br />

� ydA� 0 (5.55)<br />

where dA is a differential area parallel to the axis (Fig. 5.25), y is its distance from<br />

the axis, <strong>and</strong> the summation is taken over the entire cross section.<br />

Moment of inertia with respect to the neutral axis is given by<br />

2 I � � y dA (5.56)<br />

Values of I for several common types of cross section are given in Fig. 5.26. Values<br />

for structural-steel sections are presented in manuals of the American Institute of<br />

Steel <strong>Construction</strong>, Chicago, Ill. When the moments of inertia of other types of<br />

sections are needed, they can be computed directly by application of Eq. (5.56) or<br />

by braking the section up into components for which the moment of inertia is<br />

known.<br />

If I is the moment of inertia about the neutral axis, A the cross-sectional area,<br />

<strong>and</strong> d the distance between that axis <strong>and</strong> a parallel axis in the plane of the cross<br />

section, then the moment of inertia about the parallel axis is<br />

2<br />

I� � I � Ad (5.57)<br />

With this equation, the known moment of inertia of a component of a section about<br />

the neutral axis of the component can be transferred to the neutral axis of the<br />

complete section. Then, summing up the transferred moments of inertia for all the<br />

components yields the moment of inertia of the complete section.<br />

When the moments of inertia of an area with respect to any two perpendicular<br />

axes are known, the moment of inertia with respect to any other axis passing<br />

through the point of intersection of the two axes may be obtained through the use

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