Download ebook Engineering Construction in Steel and Timber
Download ebook Engineering Construction in Steel and Timber

Engineering Construction in Steel and Timber by William Henry Warren
Engineering Construction in Steel and Timber
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Author: William Henry Warren
Number of Pages: 116 pages
Published Date: 13 Sep 2013
Publisher: Rarebooksclub.com
Publication Country: United States
Language: Englishhttps://d20eq91zdmkqd.cloudfront.net/assets/images/book/large/9781/2976/9781297675218.jpg
Type: Pdf
ISBN: 9781230157290
File Name: engineering.construction.in.steel.and.timber.pdf
Download Link: engineering construction in steel and timber
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This historic book may have numerous typos and missing text. Purchasers can usually download a free scanned copy of the original book (without typos) from the publisher. Not indexed. Not illustrated. 1910 edition. Excerpt: ...continuous girders for various purposes. Two cases will be considered in the first instance: --1. When the load on any span is uniformly distributed over that span. 2. When the loads are concentrated at one or more points in a span. A third case might occur with both distributed and concentrated loads, but this could obviously be treated by combining the results of each loading considered separately. The assumptions made in the various examples considered in this chapter are: --1. That all the supports are on the same level or on the same uniform gradient. 2. That the girder is uniform in section throughout its length. With regard to the second assumption, which is never realised in bridges, in which the material is disposed in accordance with the variations in the stresses, the errors in the stresses need not lead to errors in the design of the various members of any practical importance. Let M0, M, M2 and M3, Fig. 271, denote the bending moments at the points of support A, B, C and D respectively. Let lv l2 and l3 be the lengths of the spans, and wv w.z and w3 denote the loads per lineal foot. Then, on the assumptions stated, it can be proved that--+ 2M1(Z, +12) + M21.2 + i(w2l23 + wj) = 0. This equation expresses the relation between the bending moments at any three consecutive piers; it is known as the equation of three moments, and was first demonstrated by Clapeyron. The moments M, and M2 in Fig. 271 tend to bend the girders upwards; thus in Fig. 270, which shows a continuous girder of three spans, the deflection over the piers B and C is upwards, and the diagram of upward bending moments is represented by the figure AicD, Fig. 271. The bending moments over the points A and D are zero. Beside the upward bending moments, which attain..

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