Worked examples involving Bending Stess and Moments of Inertia

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Please Note: Reference pages on the bending moments of beams is in preparation and will be published shortly. In the mean time the formulae for the following examples are quoted without proof.

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The General Equation for bending is used throughout. The proof of this is to be found in "Engineering/Materials/Bending Stress". For convenience the equation is written here and is as follows:

\frac{f}{y}=\frac{M}{I}=\frac{E}{R}

Where f is the stress at a distance y from the Neutral Axis

  • M is the Bending Moment
  • I is the Moment of Inertia of the section
  • E is Young's Modulus
  • R is the Radius of curvature

It is obviously important to use the same units throughout!

Example 1 [imperial]
Problem

The beam of a symmetrical I section is simply supported over a span of 30 ft.

If the maximum permissible stress is 5 tons/sq.in., what concentrated load can be carried at a distance of 10 ft from one support?

Workings
23287/Worked-Examples-0011.png

Whilst it is not stated in the question, it is normal practice to load an I-section with XX as the axis of bending. Thus the Bending Moment is in the YY plane.

If the load is W tons then the maximum Bending Moment is given by: \hat{M}=10\times\displaystyle\frac{2W}{3} or 20\times\displaystyle\frac{w}{3} i.e. Maximum Bending Moment =\displaystyle\frac{20\;W}{3}\;ton - ft=80\;W\;ton - in

23287/Worked-Examples-0012.png

Using the method for establishing the Moment of Area of an I-section beam shown in "Engineering/Materials/Bending"

I =2 \left [4\times\frac{0.46^3}{12} + 4\times0.46(4.5 - \frac{0.46}{2})^2 \right] + \frac{(0.3\times8.08^3)}{12} = 2 \left [0.032 + 33.4\right ] + 12.5 = 79.4\;in^4

Using the General equation of Bending \frac{5}{4.5} = \frac{80\;W}{79.4} \therefore\;\;\;\;\;W = \frac{(5\times79.4)}{(4.5\times80)} = 1.1\,tons

Solution
  • W=1.1\;tons