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Building Design and Construction Handbook - Merritt - Ventech!

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STRUCTURAL THEORY 5.15<br />

loaded with p s, <strong>and</strong> also with the windward wide unloaded <strong>and</strong> the leeward side<br />

carrying 1.5p s.<br />

For curved roofs, the snow load on the portion that is steeper than 70p� may<br />

be taken as zero. For the less-steep portion, the load p s may be computed as for a<br />

sloped roof, with � taken as the angle with the horizontal of a line from the crown<br />

to points on the roof where the slope starts to exceed 70�. Curved roofs should be<br />

designed with the whole area fully loaded with p s. They also should be designed<br />

for the case of snow only on the leeward side, with the load varying uniformly<br />

from 0.5p s at the crown to 2p s at points where the roof slope starts to exceed 30�<br />

<strong>and</strong> then decreasing to zero at points where the slope starts to exceed 70�.<br />

Multiple folded-plate, sawtooth, <strong>and</strong> barrel-vault roofs similarly should be<br />

designed for unbalanced loads increasing from 0.5p s at ridges to 3p s in valleys.<br />

Snow drifts may form on a roof near a higher roof that is less than 20 ft<br />

horizontally away. The reason for this is that wind may blow snow from the higher<br />

roof onto the lower roof. Drifts also may accumulate at projections above roofs,<br />

such as at parapets, solar collectors, <strong>and</strong> penthouse walls. Drift loads accordingly<br />

should be taken into account when:<br />

1. The ground snow load p g exceeds 10 lb/ft 2 .<br />

2. A higher roof exists (or may be built in the future) within 20 ft of the building,<br />

if the height differential, ft, exceeds 1.2p ƒ/�, where p ƒ is computed from Eq.<br />

(5.16) <strong>and</strong> � is the snow density, lb/ft 3 .<br />

3. A projection extends a distance, ft, exceeding 1.2p ƒ/� above the roof <strong>and</strong> is<br />

more than 15 ft long.<br />

In computation of drift loads, the snow density �, lb/ft 3 , may be taken as follows:<br />

p � 11–30 31–60 60 or more<br />

g<br />

� � 15 20 25<br />

The drift may be assumed to be a triangular prism with maximum height, located<br />

adjacent to a higher roof or along a projection, taken as h d � 2p g/�, modified by<br />

factors for risk <strong>and</strong> exposure, described for flat roofs. Width of the prism should<br />

be at least 10 ft <strong>and</strong> may be taken as 3h d for projections up to 50 ft long <strong>and</strong> as<br />

4h d for projections more than 50 ft long. Accordingly, the load varies uniformly<br />

with distance from a projection, from h d� at the projection to zero. For drifts due<br />

to snow load from a higher roof at a horizontal distance S, fit, away horizontally<br />

(S � 20 ft), the maximum drift intensity may be taken as h d�(20 � S)/20.<br />

Rain-Snow Load Combination. In roof design, account should be taken of the<br />

combination of the design snow load with a temporary water load from an intense<br />

rainstorm, including the effects of roof deflection on ponding. The added water load<br />

depends on the drainage characteristics of the roof, which, in turn, depend on the<br />

roof slope. For a flat roof, the rain surcharge may be taken as 8 lb/ft 2 for slopes<br />

less 1 ⁄4 in/ft <strong>and</strong> as 5 lb/ft 2 for steeper slopes, except where the minimum allowable<br />

design snow load p exceeds p computed from Eq. (5.16). In such cases, these<br />

min ƒ<br />

water surcharges may be reduced by p � p .<br />

min ƒ<br />

(W. Tobiasson <strong>and</strong> R. Redfield, ‘‘Snow Loads for the United States,’’ Part II,<br />

<strong>and</strong> S. C. Colbeck, ‘‘Snow Loads Resulting from Rain on Snow,’’ U.S. Army Cold<br />

Regions Research <strong>and</strong> Engineering Laboratory, Hanover, N.H.)

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