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Theory of Structures

Theory of Structures
For beams breadth is constant,

Depth d 1/M
Depth d M
Depth d 3
Depth d

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Theory of Structures
Inertia of a rectangular section of width and depth about an axis passing the moment of through C.G. and parallel to its width is

BD²/6
BD³/6
B²D/6
BD³/12

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Theory of Structures
Y are the bending moment, moment of inertia, radius of curvature, modulus of If M, I, R, E, F, and elasticity stress and the depth of the neutral axis at section, then

M/I = E/R = F/Y
I/M = R/E = F/Y
M/I = R/E = F/Y
M/I = E/R = Y/F

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Theory of Structures
Beams composed of more than one material, rigidly connected together so as to behave as one piece, are known as

Indeterminate beams
Determinate beams
Composite beams
Compound beams

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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

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

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Theory of Structures
The locus of reaction of a two hinged semi-circular arch, is

Hyperbola
Circle
Parabola
Straight line

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