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Theory of Structures

Theory of Structures
Stress may be defined as

None of these
Force per unit volume
Force per unit length
Force per unit area

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Theory of Structures
A simply supported beam carries varying load from zero at one end and w at the other end. If the length of the beam is a, the maximum bending moment will be

wa/27
w²a
wa²
wa²/27

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Theory of Structures
The locus of the end point of the resultant of the normal and tangential components of the stress on an inclined plane, is

Ellipse
Circle
Straight line
Parabola

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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 = S – F
Q = S × F
Q = F – S

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Theory of Structures
In a shaft, the shear stress is not directly proportional to

Length of the shaft
Radius of the shaft
Modulus of rigidity
Angle of twist

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Theory of Structures
A square column carries a load P at the centroid of one of the quarters of the square. If a is the side of the main square, the combined bending stress will be

4p/a²
2p/a²
3p/a²
p/a²

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