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Theory of Structures

Theory of Structures
A body is said to be in equilibrium if

None of these
It rotates about its C.G.
It moves vertically
It moves horizontally

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Theory of Structures
The moment of inertia of a triangular section (height h, base b) about its base, is

b³h/12
bh²/12
bh³/12
b²h/12

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

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Theory of Structures
A cantilever of length ‘L’ is subjected to a bending moment ‘M’ at its free end. If EI is the flexural rigidity of the section, the deflection of the free end, is

ML²/3EI
ML/EI
ML²/2EI
ML/2EI

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

1.2
1.5
1.7
1.3

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Theory of Structures
H V are the algebraic sums of the forces resolved horizontally and vertically respectively, M is the algebraic sum of the moments of forces about any point, for the equilibrium of the body acted upon

V = 0
M = 0
All of these
H = 0

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