Bending Stress and Shear Stress
Flexural Formula | Assumptions in Simple Bending |
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M = σ * I / y M = Maximum Bending moment (moment of resistance of a beam) I = Moment of inertia of the beam section about the neutral axis y = Distance of the layer from the neutral axis E = Modulus of elasticity of the beam material R = Radius of curvature of a bent beam |
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Shear Stress Distribution for Circular Beam Section
The shear stress distribution diagram for a circular beam section can be represented as follows:
alt="Shear Stress Distribution for Circular Beam Section">Formula to calculate average shear stress for a circular section with diameter 'd':
τ_avg = (3/4) * τ_max
Shear Stress Distribution for Rectangular Beam Section
The shear stress distribution diagram for a rectangular beam section can be represented as follows:
" alt="Shear Stress Distribution for Rectangular Beam Section">Formula to calculate average shear stress for a rectangular section:
τ_avg = (2/3) * τ_max
Shear Stress for Beam
Shear stress (τ) for a beam can be calculated using the formula:
τ = (Shear Force * Distance to Centroid of Shear Area) / (Shear Area * Shear Width)
Shear Distribution Diagram for T and C Sections
Here is the shear distribution diagram for T and C sections:
" alt="Shear Distribution Diagram for T and C Sections">Simple Bending
Term | Explanation |
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Neutral Axis | The fibers in the lower part of the beam undergo elongation while those in the upper part are shortened. These changes in the lengths of the fibers set up tensile and compressive stresses in the fibers. The fibers in the centroidal layer are neither shortened nor elongated. These centroidal layers which do not undergo any extension or compression is called neutral layer or neutral surface. When the beam is subjected to pure bending, there will always be one layer which will not be subjected to either compression or tension. This layer is called the neutral layer, and the axis passing through this layer is called the neutral axis. |
Moment of Resistance | Moment of resistance refers to the resistance offered by a beam to bending. It is the measure of a beam's ability to resist the bending moment applied to it. The moment of resistance depends on the shape, size, and material of the beam. It is directly proportional to the moment arm and the bending stress induced in the beam. The moment of resistance is a crucial parameter in the design and analysis of beams subjected to bending loads. |
Bending Types
Bending Type | Characteristics |
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Pure Bending |
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Ordinary Bending |
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