Structure deformation and inclined sections

Mechanics

Stiffness and deformation

\[F = k\delta\]

Where

  • \(F\) is force
  • \(k\) is stiffness
  • \(\delta\) is deformation
\[\delta = \frac{FL}{EA}\]
  • \(\delta\) is deformation
  • \(F\) is force
  • \(L\) is length
  • \(E\) is Young’s Modulus
  • \(A\) is area

If non-uniform loading:

\[\delta_i = \frac{N_i L_i}{EA}\]

Where

  • \(N_i\) is an internal force
  • \(L_i\) is length from reference where the internal force is measured

Note: you need to consider ALL forces in the beam that act in the same axis of deformation.

In differential form:

\[d\delta = \frac{N(x) dx}{E A(x)}\]

Stresses on inclined sections

\[\sigma_{\theta} = \frac{F}{A} \cos^2{\theta}\]

Where

  • \(\sigma_{\theta}\) is normal stress on angle \(\theta\)
  • \(F\) is force
  • \(A\) is area
  • \(\theta\) is angle of inclination
\[\tau_{\theta} = -\frac{F}{A} \sin{\theta} \cos{\theta}\]

Where \(\tau_{\theta}\) is shear stress on angle \(\theta\)