The stress, strain, dimension, curvature, elasticity, are all related, under certain assumption, by the theory of simple bending.   This theory relates to beam flexure resulting from couples applied to the beam without consideration of the shearing forces.

The superposition principle is one of the most important tools for solving beam loading problems allowing simplification of very complicated design problems..

For beams subjected to several loads of different types the resulting shear force, bending moment, slope and deflection can be found at any location by summing the effects due to each load acting separately to the other loads.

e = strain
E = Young's Modulus = σ /e (N/m²)
y = distance of surface from neutral surface (m).
R = Radius of neutral axis (m).
I = Moment of Inertia (m⁴ - more normally cm⁴)
Z = section modulus = I/y_max(m³ - more normally cm³)
F = Force (N)
x = Distance along beam
δ = deflection (m)
θ = Slope (radians)
σ = stress (N/m²)

A straight bar of homogeneous material is subject to only a moment at one end and an equal and opposite moment at the other end...

The beam is symmetrical about Y-Y
The traverse plane sections remain plane and normal to the longitudinal fibres after bending (Beroulli's assumption)
The fixed relationship between stress and strain (Young's Modulus)for the beam material is the same for tension and compression ( σ= E.e )


Consider two section very close together (AB and CD).
After bending the sections will be at A'B' and C'D' and are no longer parallel.   AC will have extended to A'C' and BD will have compressed to B'D'
The line EF will be located such that it will not change in length.   This surface is called neutral surface and its intersection with Z_Z is called the neutral axis
The development lines of A'B' and C'D' intersect at a point 0 at an angle of θ radians and the radius of E'F' = R
Let y be the distance(E'G') of any layer H'G' originally parallel to EF..Then

H'G'/E'F' =(R+y)θ /R θ = (R+y)/R

And the strain e at layer H'G' =

e = (H'G'- HG) / HG = (H'G'- HG) / EF = [(R+y)θ - R θ] /R θ = y /R

The accepted relationship between stress and strain is σ= E.e Therefore

σ = E.e = E. y /R
σ / E = y / R

Therefore, for the illustrated example, the tensile stress is directly related to the distance above the neutral axis.   The compressive stress is also directly related to the distance below the neutral axis.   Assuming E is the same for compression and tension the relationship is the same.

As the beam is in static equilibrium and is only subject to moments (no vertical shear forces) the forces across the section (AB) are entirely longitudinal and the total compressive forces must balance the total tensile forces.  The internal couple resulting from the sum of ( σ.dA .y) over the whole section must equal the externally applied moment.

This can only be correct if Σ(yδa) or Σ(y.z.δy) is the moment of area of the section about the neutral axis.  This can only be zero if the axis passes through the centre of gravity (centroid) of the section.

The internal couple resulting from the sum of ( σ.dA .y) over the whole section must equal the externally applied moment.  Therefore the couple of the force resulting from the stress on each area when totalled over the whole area will equal the applied moment

From the above the following important simple beam bending relationship results

It is clear from above that a simple beam subject to bending generates a maximum stress at the surface furthest away from the neutral axis.  For sections symmetrical about Z-Z the maximum compressive and tensile stress is equal.

σ_max = y_max. M / I

The factor I /y_max is given the name section Modulus (Z) and therefore

σ_max = M / Z

Values of Z are provided in the tables showing the properties of standard steel sections

Below is shown the arc of the neutral axis of a beam subject to bending.

For small angle dy/dx = tan θ = θ
The curvature of a beam is identified as dθ /ds = 1/R
In the figure δθ is small and δx; is practically = δs; i.e ds /dx =1

From this simple approximation the following relationships are derived.

Integrating between selected limits.

The deflection between limits is obtained by further integration.

It has been proved ref Shear - Bending that dM/dx = S and dS/dx = -w = d²M /dx
Where S = the shear force M is the moment and w is the distributed load /unit length of beam.   therefore

If w is constant or a integratatable function of x then this relationship can be used to arrive at general expressions for S, M, dy/dx, or y by progressive integrations with a constant of integration being added at each stage.  The properties of the supports or fixings may be used to determine the constants. (x= 0 - simply supported, dx/dy = 0 fixed end etc )

In a similar manner if an expression for the bending moment is known then the slope and deflection can be obtained at any point x by single and double integration of the relationship and applying suitable constants of integration.

Singularity functions can be used for determining the values when the loading a not simple ref Singularity Functions

Consider a cantilever beam (uniform section) with a single concentrated load at the end.  At the fixed end x = 0, dy = 0 , dy/dx = 0

From the equilibrium balance ..At the support there is a resisting moment -FL and a vertical upward force F.
At any point x along the beam there is a moment F(x - L) = M_x = EI d ²y /dx ²

Consider a simply supported uniform section beam with a single load F at the centre.    The beam will be deflect symmetrically about the centre line with 0 slope (dy/dx) at the centre line.   It is convenient to select the origin at the centre line.

This is a method of determining the change in slope or the deflection between two points on a beam.  It is expressed as two theorems...

Theorem 1
If A and B are two points on a beam the change in angle (radians) between the tangent at A and the tangent at B is equal to the area of the bending moment diagram between the points divided by the relevant value of EI (the flexural rigidity constant).

Theorem 2
If A and B are two points on a beam the displacement of B relative to the tangent of the beam at A is equal to the moment of the area of the bending moment diagram between A and B about the ordinate through B divided by the relevant value of EI (the flexural rigidity constant).

The bending moment at A = M_A = FL
The area of the bending moment diagram A_M = F.L² /2
The distance to the centroid of the BM diagram from B= x_c = 2L/3
The deflection of B = y _b = A _M.x _c /EI = F.L ³ /3EI
The slope at B relative to the tan at A = θ _b =A_M /EI = FL² /2EI

E = 210 GPa ......I = 834 cm⁴...... EI = 1,7514. 10 ⁶Nm ²

A₁ = 10.1,8.1,8/2 = 16,2kNm
A₂ = 10.1,8.2 = 36kNm
A₂ = 10.1,8.2 = 36kNm
A₁ = 10.1,8.1,8/2 = 16,2kNm
x₁ = Centroid of A₁ = (2/3).1,8 = 1,2
x₂ = Centroid of A₂ = 1,8 + 1 = 2,8
x₃ = Centroid of A₃ = 1,8 + 1 = 2,8
x₄ = Centroid of A₄ = (2/3).1,8 = 1,2

θ_A = (A₁ + A₂) /EI   =   (16,2+36).10 ³ / (1,7514. 10 ⁶)
=  0,029rads   =   1,7 degrees

δ_C = (A_M.x_M) /EI   =   (A₁ x₁ +A₂ x₂) / EI   =   120,24.10 ³/ (1,7514. 10 ⁶)
=   0,0686m = 68,6mm