Strength of materials — beam flexure terminology: What is the name given to the product of Young's modulus (E) and the second moment of area (I) of a beam cross-section?

Difficulty: Easy

Correct Answer: Flexural rigidity

Explanation:


Introduction / Context:
In strength of materials, the bending stiffness of a prismatic beam is governed by both the material's elastic property and the cross-sectional geometry. The compound quantity that measures this bending stiffness is the product E * I, widely used in deflection and slope calculations.



Given Data / Assumptions:

  • E = Young's modulus (material stiffness in tension/compression).
  • I = second moment of area about the neutral axis (geometric stiffness in bending).
  • Small deflection theory (Euler–Bernoulli) is assumed.


Concept / Approach:
Beam curvature under bending follows M / I = E / R, which rearranges to M = (E * I) / R. The larger the product E * I, the smaller the curvature R for a given bending moment M. Hence E * I quantifies resistance to bending and is termed flexural rigidity.



Step-by-Step Solution:

Start from bending equation: M / I = E / R.Rearrange: M = (E * I) / R.Interpretation: For fixed M, higher E * I implies larger R (flatter curve) → stiffer in bending.Therefore, E * I is called flexural rigidity.


Verification / Alternative check:
Deflection formulas for standard cases (e.g., simply supported beam with central load) contain E * I in the denominator, confirming that deflection decreases as E * I increases.



Why Other Options Are Wrong:

  • Bulk modulus: volumetric elasticity, unrelated to flexure directly.
  • Torsional rigidity: G * J for twisting, not bending.
  • Modulus of rigidity: the shear modulus G alone, not multiplied by I.
  • Section modulus: geometric term Z = I / y, not multiplied by E.


Common Pitfalls:
Confusing section modulus Z with second moment I; only E * I represents flexural rigidity.



Final Answer:
Flexural rigidity

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