How is Elastic Energy of a Bent Steel Rod Approximated?

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SUMMARY

The discussion centers on approximating the elastic energy of a bent steel rod using the formula U[y]= ∫(0 to L) (1/2)YI(y'')² dz. The key variables include Young's modulus (Y), the moment of inertia (I), and the radius of curvature (R). Participants clarify that the rod can be treated as a curve y(z), and the radius of curvature can be derived from the mathematical definition. The challenge lies in understanding how to relate the infinitesimal length of the rod to its curvature and energy expression.

PREREQUISITES
  • Understanding of elastic energy concepts in materials science.
  • Familiarity with Young's modulus and its significance in material properties.
  • Knowledge of moment of inertia and its calculation for different cross-sections.
  • Basic calculus, particularly differentiation and integration of functions.
NEXT STEPS
  • Research the mathematical definition of the radius of curvature for curves.
  • Study the derivation of elastic energy formulas in mechanics of materials.
  • Explore the relationship between curvature and bending in beams and rods.
  • Learn about the applications of Young's modulus in engineering design and analysis.
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Students in physics and engineering, particularly those studying mechanics of materials, as well as professionals involved in structural analysis and design of steel components.

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Homework Statement


[Math. for Physicists, M. Stone Problem 1.4]

Assume that a rod of length L is only slightly bent into the yz plane and lies close to the z axis, show that the elastic energy can be approximated as
U[y]= \int_{0}^{L} \frac{1}{2}YI(y'')^2 dz

Homework Equations



It is given that the elastic energy per unit length of a bent rod , u=\frac{1}{2}YI/R^{2}
R is the radius of curvature due to the bending, Y is the Young's modulus of the steel and I is the moment of inertia of the rod's cross section about an axis through its centroid and
perpendicular to the plane in which the rod is bent.

The Attempt at a Solution



I don't quite get the picture.
Does it mean that each infinitesimal piece is a segment of a circle R with a different center? Or should I consider the whole bent rod as a segment of a circle of radius R?

But still the infinitesimal rod length should be \sqrt{1+(y')^2} dz, so how can I get y''^2?

Thank you very much!



The Attempt at a Solution

 
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