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Strength of Materials
Standard Equation

Beam Bending Stress Equation

Calculates the normal bending stress in a straight beam subjected to transverse loading and bending moments.

Primary Mathematical Expression

\sigma = M * y / I

Design Schematic

Bearing ABearing BPulley 1F1Gear SeatF_mesh (Bending)KeywayTorque (T)Fillet Shoulders

Nomenclature & Variables

SymbolVariable NameMetric UnitImperial UnitDescription
MBending momentN·min·lbThe applied bending moment acting on the cross-section.
yDistance to neutral axismminDistance from neutral axis to the point of interest.
IArea moment of inertiamm⁴in⁴The geometric stiffness property of the cross-section.
\sigmaBending stressMPapsiThe resulting normal stress at distance y.

Step-by-Step Derivation

  1. 1

    Consider a straight beam subjected to pure bending moments. The bending moment causes deformation where top fibers contract and bottom fibers stretch.

  2. 2

    The axial strain at any fiber is proportional to its distance from the neutral surface: \epsilon = -y / \rho, where \rho is the radius of curvature.

  3. 3

    Assuming elastic behavior, Hooke's Law applies: \sigma = E * \epsilon = -E * y / \rho.

  4. 4

    The internal bending moment must balance the external moment: M = \int -\sigma * y * dA = \int (E * y² / \rho) * dA = (E / \rho) * I.

  5. 5

    Substituting E / \rho = M / I back into the stress equation yields the bending stress formula: \sigma = M * y / I.

Worked Example Calculation

Problem Statement

A rectangular steel beam undergoes a bending moment of 1200 N·m. The distance from the neutral axis to the outer fiber is 25 mm, and the area moment of inertia of the cross-section is 1.6 \times 10^5 mm⁴. Calculate the maximum bending stress.

Calculation Steps
  • Identify input parameters: M = 1200 N·m = 1,200,000 N·mm, y = 25 mm, I = 160,000 mm⁴.
  • Apply the Bending Stress Formula: \sigma = M * y / I.
  • Compute: \sigma = (1,200,000 * 25) / 160,000 = 30,000,000 / 160,000 = 187.5 MPa.
Final ResultBending Stress = 187.5 MPa

Engineering Assumptions

  • The beam material is homogeneous, isotropic, and obeys Hooke's Law.
  • The beam is straight with a uniform cross-section.
  • Plane sections remain plane after bending (Bernoulli-Euler hypothesis).
  • The loading is applied in the plane of symmetry.

Design Limitations

  • Not applicable for short, deep beams where shear deformation is significant (requires Timoshenko beam theory).
  • Not applicable beyond the material's elastic limit (yield strength).
  • Does not account for stress concentration zones near holes, fillets, or notches.

Academic References & Standards

ASTM A36standard

Standard Specification for Carbon Structural Steel

The standard detailing carbon steel structural shapes.

Shigley Ch 3textbook

Shigley's Mechanical Engineering Design, 11th Edition

Textbook covering bending and normal stresses in mechanical components.