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Theory of Structures

Theory of Structures
The ratio of the area of cross-section of a circular section to the area of its core, is

16
14
15
11

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Theory of Structures
A steel plate d × b is sandwiched rigidly between two timber joists each D × B/2 in section. The steel will be (where Young’s modulus of steel is m times that of the timber).

BD² + mbd²)/6D]
BD² + mbd²)/4D]
BD³ + mbd³)/6D]
BD² + mbd³)/4D]

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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

W²L/AE
W²L/2AE
WL/AE
WL/2AE

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Theory of Structures
For calculating the allowable stress of long columns σ0 = σy/n [1 - a (1/r)²]is the empirical formula, known as

Perry
Straight line formula
Parabolic formula
Rankine

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Theory of Structures
The area of the core of a column of cross sectional area A, is

(1/6) A
(1/12) A
(1/3) A
(1/18) A

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Theory of Structures
In case of principal axes of a section

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

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