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Theory of Structures

Theory of Structures
For beams breadth is constant,

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

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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
B²D/6
BD³/6
BD³/12

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Theory of Structures
A steel rod 1 metre long having square cross section is pulled under a tensile load of 8 tonnes. The extension in the rod was 1 mm only. If Esteel = 2 × 106 kg/cm², the side of the rod, is

1 cm
2.5 cm
2 cm
1.5 cm

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Theory of Structures
A steel bar 5 m × 50 mm is loaded with 250,000 N. If the modulus of elasticity of the material is 0.2 MN/mm² and Poisson’s ratio is 0.25, the change in the volume of the bar is:

1.125 cm³
4.125 cm²
3.125 cm³
2.125 cm³

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Theory of Structures
Maximum principal stress theory for the failure of a material at elastic point, is known

Guest's or Trecas' theory
St. Venant's theory
Von Mises' theory
Rankine's theory

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Theory of Structures
At yield point of a test piece, the material

Regains its original shape on removal of the load
Undergoes plastic deformation
Behaves in an elastic manner
Obeys Hooke’s law

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