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Structural Concrete - Hassoun

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232 Chapter 6 Deflection and Control of Cracking<br />

and the modulus of rupture of concrete as<br />

and<br />

f r = 7.5λ √ f ′ cpsi (0.623λ √ f ′ cMPa) (6.7)<br />

M a = maximum unfactored moment in member at stage for which deflection is being computed<br />

I g = moment of inertia of gross concrete section about centroidal axis, neglecting reinforcement<br />

I cr = moment of inertia of cracked transformed section<br />

= distance from centroidal axis of cross section, neglecting steel, to tension face<br />

Y t<br />

The following limitations are specified by the code:<br />

1. For continuous spans, the effective moment of inertia may be taken as the average of the<br />

moment of inertia of the critical positive- and negative-moment sections.<br />

2. For prismatic members, I e may be taken as the value obtained from Eq. 6.5 at midspan for<br />

simple and continuous spans and at the support section for cantilevers (ACI Code, Section<br />

24.2.3.6 and 24.2.3.7).<br />

Note that I e , as computed by Eq. 6.5, provides a transition between the upper and lower<br />

bounds of the gross moment of inertia, I g , and the cracked moment of inertia, I cr , as a function<br />

of the level of M cr /M a . Heavily reinforced concrete members may have an effective moment<br />

of inertia, I e , very close to that of a cracked section, I cr , whereas flanged members may have<br />

an effective moment of inertia close to the gross moment of inertia, I g .<br />

3. For continuous beams, an approximate value of the average I e for prismatic or nonprismatic<br />

members for somewhat improved results is as follows: For beams with both ends continuous,<br />

For beams with one end continuous,<br />

AverageI e = 0.70I m + 0.15(I e1 + I e2 ) (6.8)<br />

AverageI e = 0.85I m + 0.15(I con ) (6.9)<br />

where I m is the midspan I e , I e1 , I e 2 = I e at beam ends, and I con = I e at the continuous<br />

end. Also, I e may be taken as the average value of the I e ’s at the critical positive- and<br />

negative-moment sections. Moment envelopes should be used in computing both positive<br />

and negative values of I e . In the case of a beam subjected to a single heavy concentrated<br />

load, only the midspan I e should be used.<br />

6.2.5 Properties of Sections<br />

To determine the moment of inertia of the gross and cracked sections, it is necessary to calculate<br />

the distance from the compression fibers to the neutral axis (x or kd).<br />

1. Gross moment of inertia, I g (neglect all steel in the section):<br />

a. For a rectangular section of width b and a total depth h, I g = bh 3 /12.<br />

b. For a T-section, flange width b, web width b w , and flange thickness t, calculate y, the<br />

distance to the centroidal axis from the top of the flange:<br />

y = (bt2 ∕2)+b w (h − t)[(h + t)∕2]<br />

bt + b w (h − t)<br />

(6.10)

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