
Let us consider a beam under the action of deforming forces. The beam bends into a circular arc as shown in Fig.
EXPRESSION
FOR INTERNAL BENDING MOMENT
Let
us consider a beam under the action of deforming forces. The beam bends into a
circular arc as shown in Fig 1.8. Let AB be the neutral axis of the beam. Here
the filaments above AB are elongated and the filaments below AB are compressed.
The filament AB remains unchanged.

Let PQ be the arc chosen from the neutral axis. If R is the radius of curvature of the neutral axis and θ is the angle subtended by it at its centre of curvature 'C'.
Then
we can write original length PQ = Rθ
……...(1)
Let
us consider a filament P'Q' at a distance 'x'
from the neutral axis.
∴ We can write the
extended length = P'Q' = (R+x) θ ...... (2)
From
eqn.(1) and eqn.(2), we have
Increase
in its length = P'Q' ‒ PQ
(or)
Increase in its length = (R+x) θ‒Rθ
Increase
in its length = xθ …..(3)
We
know Linear Strain = Increase in length / Original length
(or)
Linear
Strain = xθ / Rθ
Linear
Strain = x / R …….(4)
We
know, The youngs modulus of the material Y = Stress / Linear strain
(or)
Stress = Y × Linear strain …….(5)
Substituting
eqn.(4) in (5), we have
Stress
= Yx / R
If
δA is the area of cross section of the filament P'Q'. Then,
The
tensile force on the area (δA) = Stress × Area
(i.e)
Tensile Force = Yx/R . δA
We
know that, Moment of force = Force × Perpendicular Distance
∴ Moment of the tensile
force about the neutral axis AB (or) PQ = Yx/R
. δA . x
PQ
= (Y/R)δAx2
The
moment of force acting on both the upper and lower halves of the neutral axis
can be got by summing all the moments of tensile and compressive forces about
the neutral axis.
The
moment of all the forces about the neutral axis = (Y/R) Σx2δA
Here
Ig = Σx2δA = AK2
is called as the geometrical moment of inertia.
Where,
A is the total area of the beam and
K
is the radius of the Gyration.
Total
moment of all the forces (or) Internal bending moment = YIg/R ………..(6)
SPECIAL CASES
(I) RECTANGULAR CROSS
SECTION
If
'b' is the breadth and 'd' is the thickness of the beam, then
Area
A = bd and K2 = d2/12
Ig
= AK2
⇒ bd.d2 / 12
⇒ bd3 / 12
Substituting
the value of Ig in eqn.(6), we can write
Bending
moment for a rectangular cross section = Ybd3 / 12R ……..(7)
(II) CIRCULAR CROSS
SECTION
For
a circular cross section if 'r' is
the radius, then Area A = πг2
and
K2 = r2/4
Ig
= AK2
Ig
= [ π r2 × r2 ]
/ 4
Ig
= πr4
/ 4
Substituting
the value of Ig, in eqn.(6), we can write
The
Bending moment of a circular cross section = πYr4 / 4R ………..(8)
Applied Physics I: Chapter 1: Properties of Matter - Elasticity : Tag: Applied Physics : - Expression for internal Bending Moment
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