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Theory of Structures

Theory of Structures
A body is said to be in equilibrium if

It moves vertically
None of these
It rotates about its C.G.
It moves horizontally

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

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Theory of Structures
If Q is load factor, S is shape factor and F is factor of safety in elastic design, the following:

Q = S + F
Q = F – S
Q = S × F
Q = S – F

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Theory of Structures
A truss containing j joints and m members, will be a simple truss if

m = 2j – 3
j = 3m – 2
j = 2m – 3
m = 3j – 2

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Theory of Structures
A simply supported beam A carries a point load at its mid span. Another identical beam B carries the same load but uniformly distributed over the entire span. The ratio of the maximum deflections of the beams A and B, will be

2/3
3/2
5/8
8/5

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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
Rankine
Parabolic formula

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