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Theory of Structures

Theory of Structures
The forces in the members of simple trusses, may be analysed by

All of these
Graphical method
Method of sections
Method of joints

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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

B²D/6
BD²/6
BD³/12
BD³/6

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Theory of Structures
In case of principal axes of a section

Difference of moment inertia is zero
Sum of moment of inertia is zero
None of these
Product of moment of inertia is zero

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Theory of Structures
The yield moment of a cross section is defined as the moment that will just produce the yield stress in

The fibre everywhere
The outer most fibre of the section
The neutral fibre of the section
The inner most fibre of the section

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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:

4.125 cm²
1.125 cm³
3.125 cm³
2.125 cm³

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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

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

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