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Theory of Structures

Theory of Structures
The maximum deflection due to a load W at the free end of a cantilever of length L and having flexural rigidity EI, is

WL3/3EI
WL3/2EI
WL²/3EI
WL²/2EI

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Theory of Structures
constant, depth of a cantilever of length of uniform strength loaded with Keeping breadth uniformly distributed load varies from zero at the free end and

l) at the fixed end
3w l at the fixed end
w l) at the fixed end
2w w l at the fixed end

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

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

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Theory of Structures
A cantilever of length 2 cm and depth 10 cm tapers in plan from a width 24 cm to zero at its free end. If the modulus of elasticity of the material is 0.2 × 106 N/mm², the deflection of the free end, is

3 mm
5 mm
2 mm
4 mm

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Theory of Structures
For beams of uniform strength, if depth is constant,

Width b M 2
Width b 1/M
Width b 3 M
Width b M

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Theory of Structures
Principal planes are subjected to

Normal stresses as well as tangential stresses
Normal stresses only
None of these
Tangential stresses only

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