Stress and Strain Caused by Bending Loads
Bending Loads
Learning Objectives:
- Review simple beam theory.
- Explain the concept of the neutral axis.
- State and apply bending equation to calculate bending stresses at any layer of a member subjected to bending stresses.
Bending Equation:
where,
M= Bending Moment
I = Moment of Inertia of the cross section about the neutral axis.
\(\sigma\) = stress
y = distance from the neutral axis
For symmetric sections, y = depth/2
E = Modulus of Elasticity
R = Radius of Curvature
This formula is called flexture formula.

Avenafatua, Public domain, via Wikimedia Commons
Neutral Axis:
At some point between these two surfaces, there must be a plane where the normal stresses and strains are zero. We call this plane the Neutral Plane (N.P.) represented in diagram by Neutral Axis (N.A.).
All layers above the neutral axis suffer compression whereas those below the neutral axis suffer tension. The amount by which a layer is compressed or stretched depends upon its position with respect to the neutral axis.
File:Beam bending.png: Gvfderivative work: TilmannR, Public domain, via Wikimedia Commons
Modulus of Section:
The section modulus of the cross-sectional shape is of significant importance in designing beams. It is a direct measure of the strength of the beam. A beam that has a larger section modulus than another will be stronger and capable of supporting greater loads.
It includes the idea that most of the work in bending is being done by the extreme fibres of the beam, ie the top and bottom fibres of the section. The distance of the fibres from top to bottom is therefore built into the calculation.
The elastic modulus is denoted by s. To calculate s, the distance (y) to the extreme fibres from the centroid (or neutral axis) must be found as that is where the maximum stress could cause failure.
Solved Example: 42-1-01
In a simple bending of beams, the stress in the beam varies:
A. Linearly
B. Parabolically
C. Hyperbolically
D. Elliptically
In simple or pure bending, the stress caused due to bending varies linearly from maximum compressive at the top most layer to maximum tensile at the bottom most layer (for sagging moment). The variation is linear.
Correct Answer: A
Solved Example: 42-1-02
Two beams, one having a square cross-section and another a circular cross-section, are subjected to the same amount of bending moment. If the cross-sectional area, as well as the material of both the beams, are the same, then
- Both the beams will experience the same amount of deformation
- The circular beam experiences more extreme flexural stress than the square one
Which of the above is/are correct?
A. 1 only
B. 2 only
C. Both 1 and 2
D. Neither 1 nor 2
- The circular cross-section will experience more flexural stress. This is because circular cross-section has less moment of inertia and hence, less resistance to bending.
- The material is the same but the stress value is not the same therefore both the beams will suffer the different amount of deformations.
Correct Answer: B
Solved Example: 42-1-03
A simply supported laterally loaded beam was found to deflect more than a specified value. Which of the following measures will reduce deflection?
A. Increase the area moment of inertia
B. Increase the span of the beam
C. Select a different material having lesser modulus of elasticity
D. Magnitude of the load to be increased.
Let's see each option individually.
- Option A: The area moment of inertia is a measure of resistance to rotation, or bending. Hence, increase area moment of inertia will increase the resistance to bending and the beam will have less deflection.
- Option B: Increasing the span increased the deflection of the beam as it is directly propertional to the span. Conceptually, now the supports are at a longer distance, hence the maximum deflection in the beam will actually increase.
- Option C: Modulus of elasticity is a ratio of stress to strain. Lesser modulus of elasticity means higher stress for same deflection, or in other words more strain for same stress.
- Option D: Obviously wrong as higher load will create higher deflection.
Correct Answer: A
Solved Example: 42-1-04
A beam will be in pure bending under a:
A. Constant shear force and a constant bending moment
B. Constant shear force and zero bending moment
C. Constant bending moment and zero shear force
D. None of the above
One of the assumptions of pure bending theory is the bending moment is uniform and there are no shear forces applied. Due to bending, the layers of beam eventually undergo shear stresses, but those are induced shear stresses rather than applied shear stresses.
Correct Answer: C
Solved Example: 42-1-05
A simply supported beam of span length 6 m and 75 mm diameter carries a uniformly distributed load of 1.5 kN/m. What is the value of maximum bending stress?
A. 162.98 MPa
B. 325.95 MPa
C. 625.95 MPa
D. 651.90 MPa
\[\sigma_b = \dfrac{M y}{I}\] \[M = \mathrm{Max.\ Bending\ Moment} = 6.75\ \mathrm{KN.m}\] \begin{align*} y &= \dfrac{h}{2} = \dfrac{75}{2} = 37.5\ \mathrm{mm}\\ I &= \dfrac{\pi D^4}{64} = \dfrac{\pi (75)^4}{64}\ {\mathrm{mm}}^4 \\ \sigma_b &= \dfrac{6.75 \times 10^6 \times 64 \times 37.5}{\pi \times 75^4} = 162.97\ \mathrm{MPa} \end{align*}
Correct Answer: A
Solved Example: 42-1-06
A wire of circular cross-section of diameter 1 mm is bent into a circular arc of radius 1 m by application of pure bending moments at its ends. The Young’s modulus of the material of the wire is 100 GPa. The maximum tensile stress developed in the wire, in MPA, is:
A. 25
B. 50
C. 75
D. 100
\[\dfrac{M}{I} = \dfrac{\sigma}{y} = \dfrac{E}{R}\] \begin{align*} \sigma &= \dfrac{E \cdot y}{R}\\ &= \dfrac{100 \times 10^9 \times 0.5 \times 10^{-3}}{1}\\ &= 50 \times 10^6\ \mathrm{Pa}\\ &= 50\ \mathrm{MPa} \end{align*}
Correct Answer: B
Solved Example: 42-1-07
In a simple bending theory, one of the assumption is that the material of the beam is isotropic. This assumption means that the:
A. Normal stress remains constant in all directions
B. Normal stress varies linearly in the material
C. Elastic constants are same in all the directions
D. Elastic constants varies linearly in the material
Isotropic materials that have material properties identical in all directions.
Anisotropic materials are materials whose properties are directionally dependent. Properties such as Young's Modulus, change with direction along the object. Common examples of anisotropic materials are wood and composites.
Correct Answer: C
Solved Example: 42-2-01
The neutral axis of the cross-section a beam is that axis at which the bending stress is:
A. 0
B. Min
C. Max
D. $\infty$
The axial stress is zero on the neutral surface and increases linearly as one moves away from the neutral axis.
Correct Answer: A
Solved Example: 42-3-01
A beam of uniform strength has:
A. Same cross-section throughout the beam
B. Same bending stress at every section
C. Same bending moment at every section
D. Same shear stress at every section
In general, beams have uniform cross section throughout their length. When they are loaded, there is a variation in bending moment from section to section along the length. The stress in extreme outer fibre (top and bottom) also vary from section to section along their length. The extreme fibres can be loaded to the maximum capacity of permissible stress (say $\sigma_{max}$), but they are loaded to less capacity. Hence, in beams of uniform cross section there is a considerable waste of material. When a beam is suitably designed such that the extreme fibres are loaded to the same maximum permissible bending stress by varying the cross section it will be known as a beam of uniform strength.
Correct Answer: B
Solved Example: 42-3-02
Find the section modulus of a circular section whose section diameter is 28 mm.
A. 2155
B. 6310
C. 1177
D. 650
\[ Z = \dfrac{\pi d^3}{32} = \dfrac{\pi (28)^3}{32} = 2155.1\ mm^3\]
Correct Answer: A