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Lightweight Concrete for High Strength - Expanded Shale & Clay

Lightweight Concrete for High Strength - Expanded Shale & Clay

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The value b’ was taken as the minimum web thickness of the girder which was 6 inches <strong>for</strong> an<br />

AASHTO Type II. The code specifies that d, the distance from the topmost compression fiber to<br />

the centroid of the prestressing strands need not be less than 0.8*h where h is the total depth of<br />

the composite girder. The value of d normally exceeded the minimum 0.8*h. V i and M max were<br />

the maximum moment and shear at the section in question. The lightweight concrete factor, λ,<br />

having a value of 0.85 was included in the equation based on the use of HSLC. The concrete<br />

strength f c ’ was listed in psi. Calculation of the cracking moment was accomplished with<br />

AASHTO equation (5.3):<br />

M<br />

cr<br />

'<br />

I fc<br />

= (6λ<br />

+ f<br />

Y 1000<br />

where f pe is the compressive stress at the extreme tensile fiber due to effective prestressing <strong>for</strong>ce<br />

and f d if the tensile stress at the extreme tensile fiber due to the dead load of the girder and slab.<br />

t<br />

pe<br />

−<br />

f<br />

d<br />

)<br />

(5.3)<br />

The composite section properties were used in calculating M cr . The concrete strength, f c ’, was<br />

based on cylinder tests at the time of girder testing.<br />

The web shear strength was calculated using AASHTO (1996) equation (5.4):<br />

'<br />

fc<br />

V<br />

cw<br />

= (3.5λ<br />

+ 0.3 f<br />

pc)<br />

b'<br />

d + V<br />

1000<br />

where f pc is the average compressive stress in the concrete due to effective prestressing <strong>for</strong>ce and<br />

V p is the vertical component of the effective prestressing <strong>for</strong>ce.<br />

p<br />

(5.4)<br />

ACI 11.4.2.2 provides an alternate technique <strong>for</strong> calculating V cw that was investigated in<br />

this evaluation. The ACI Code states that V cw shall be computed as the shear <strong>for</strong>ce<br />

corresponding to dead load plus live load that results in a principal tension stress of 4λ(f c ’) 1/2 at<br />

the centroidal axis of the member. In composite members, the principal tensile stress is<br />

computed using the cross section that resists live load. Lin and Burns (1981) addressed this<br />

alternate technique and provided the following equations which come directly from the<br />

application of Mohr’s circle:<br />

5-20

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