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Theory of Structures

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

BD³/6
BD³/12
BD²/6
B²D/6

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Theory of Structures
A square column carries a load P at the centroid of one of the quarters of the square. If a is the side of the main square, the combined bending stress will be

p/a²
3p/a²
2p/a²
4p/a²

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Theory of Structures
At any point of a beam, the section modulus may be obtained by dividing the moment of inertia of the section by

Depth of the neutral axis
Depth of the section
Maximum compressive stress at the section
Maximum tensile stress at the section

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Theory of Structures
Stress may be defined as

None of these
Force per unit volume
Force per unit length
Force per unit area

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Theory of Structures
A shaft rotating N.R.M. under a torque T, transmits a power

/30 Newton metres/sec
/30 Newton metres/min
/60 Newton metres/sec
/60 Newton metres/min

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Theory of Structures
A shaft subjected to a bending moment M and a torque T, experiences

Both A and B
Maximum bending stress = 32M/πd³
Neither A nor B
Maximum shear stress = 16 T/πd³

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