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Theory of Structures

Theory of Structures
The maximum magnitude of shear stress due to shear force F on a rectangular section of area A at the neutral axis, is

2F/3A
3F/2A
F/A
F/2A

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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)

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

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Theory of Structures
constant, depth of a cantilever of length of uniform strength loaded with Keeping breadth uniformly distributed load varies from zero at the free end and

3w l at the fixed end
l) at the fixed end
w l) at the fixed end
2w w l at the fixed end

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Theory of Structures
A bar L metre long and having its area of cross-section A, is subjected to a gradually applied tensile load W. The strain energy stored in the bar is

WL/2AE
WL/AE
W²L/2AE
W²L/AE

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

bh³/12
b²h/12
bh²/12
b³h/12

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Theory of Structures
If a three hinged parabolic arch, (span l, rise h) is carrying a uniformly distributed load w/unit length over the entire span,

B.M. will be zero throughout
S.F. will be zero throughout
Horizontal thrust is wl2/8h
All of these

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