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Theory of Structures

Theory of Structures
Gradually applied static loads do not change with time their

All of these
Point of application
Direction
Magnitude

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

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

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Theory of Structures
In case of principal axes of a section

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

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Theory of Structures
A simply supported rolled steel joist 8 m long carries a uniformly distributed load over it span so that the maximum bending stress is 75 N/mm². If the slope at the ends is 0.005 radian and the value of E = 0.2 × 106 N/mm², the depth of the joist, is

300 mm
200 mm
250 mm
400 mm

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Theory of Structures
Total strain energy theory for the failure of a material at elastic limit, is known

Rankine’s theory
Guest’s or Trecas’ theory
Haig’s theory
St. Venant’s theory

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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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