# Moments of Area

The calculation of deflections using Moments of Area

**Contents**

## Overview

The drawing shows the Bending Moment diagram and the shape of a deflected beam between two point and .##### MISSING IMAGE!

**23287/MoA-020.png** cannot be found in /users/23287/MoA-020.png. Please contact the submission author.

A

**beam**is a horizontal structural element that is capable of withstanding load primarily by resisting bending. The bending force induced into the material of the beam as a result of the external loads, own weight, span and external reactions to these loads is called a**bending moment**.The tangents at and to the elastic line, cut off an intercept on .
Integrating between and
If is a constant then

i.e. The

If is the radius of curvature of the beam at some point between and , then the angle between the tangents at the end of a short length where .
**increase of slope**between any two points on a beam is equal to the net area of the Bending Moment diagram between those two points divided by .The intercept of these tangents on is and since the slope everywhere is small:
Integrating
(If is a constant)

i.e. The

Account has to be taken of positive and negative areas and frequently it is convenient to break down the Bending Moment diagram into a number of simple figures, so that the moment is obtained from
The interecept is positive when the tangent at strikes below the tangent at .
This method is only used for particular applications in which it produces a quicker solution than the mathematical treatment. These cases can generally be labeled as those for which a point of zero slope is known. If this point is chosen as and is taken through then equation (2) reduces to :
Slope at =
And equation (3) gives the deflection of relative to as
**intercept on a given line**between the tangents to the beam at any two points and is equal to the net moment about that line of the Bending Moment diagram between and divided by .**Deflection**is a term that is used to describe the degree to which a structural element is displaced under a load.

i.e. The

**deflection at any point**can be found by working between there and a point of zero slope and taking Moments about the point where the deflection is required.##### MISSING IMAGE!

**23287/MoA-021.png** cannot be found in /users/23287/MoA-021.png. Please contact the submission author.

## Summarising The Cases In Which This Method Is Useful,

A

**cantilever**is a beam anchored at only one end. The beam carries the load to the support where it is resisted by moment and shear stress. Cantilever construction allows for overhanging structures without external bracing.- Most Cantilever cases ( Zero slope at the fixed end)
- Symmetrically loaded simply supported beams ( The slope at the centre is zero)
- Built in Beams ( Zero slope at each ends)

## Uniformly Distributed Loads

For uniformly distributed loads the Bending Moment diagram is a parabola and the following properties of area and centroids should be known.##### MISSING IMAGE!

**23287/MoA-022.png** cannot be found in /users/23287/MoA-022.png. Please contact the submission author.

In the above diagram the surrounding rectangle has an area of bd. and the parabola is tangential to the base.
Then

Example:

[imperial]

##### Example - Example 1

Problem

Obtain

**expressions**for the**maximum slope and deflection**of a simply supported beam of span with:- a) A concentrated load at the centre.
- b) With a uniformly distributed load over the whole length.

Workings

In both cases, by symmetry the slope is zero at the centre and the maximum slope and deflection can be found from the area of the Bending Moment diagram over half the beam. i.e. is at the support and is at the centre of the beam.

- a) If is the area of the Bending Moment diagram for half the beam then:

- b) The area of the shaded area of the Bending Moment diagram is given by:

Solution

- a) The
**slope**is and the**deflection**is - b) The
**slope**is and the**deflection**is