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Theory of Structures

Theory of Structures
In plastic analysis, the shape factor for a circular section, is

1.3
1.7
1.5
1.2

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Theory of Structures
The general expression for the B.M. of a beam of length l is the beam carries M = (wl/2) x – (wx²/2)

An isolated load at mid span
None of these
A uniformly distributed load w/unit length
A load varying linearly from zero at one end to w at the other end

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Theory of Structures
For beams of uniform strength, if depth is constant,

Width b 3 M
Width b 1/M
Width b M 2
Width b M

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Theory of Structures
In case of a simply supported I-section beam of span L and loaded with a central load W, the length of elasto-plastic zone of the plastic hinge, is

L/4
L/5
L/3
L/2

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Theory of Structures
The yield moment of a cross section is defined as the moment that will just produce the yield stress in

The fibre everywhere
The inner most fibre of the section
The outer most fibre of the section
The neutral fibre of the section

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Theory of Structures
A simply supported beam A carries a point load at its mid span. Another identical beam B carries the same load but uniformly distributed over the entire span. The ratio of the maximum deflections of the beams A and B, will be

3/2
2/3
5/8
8/5

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