The intensity of horizontal shear stress at the elemental part of a beam section
Answers
Analysis of Horizontal Shearing Stress
In this section, fv will be used for shearing
stress instead of the standard symbol τ.
For the upper shaded portion of the beam, the forces acting are the total normal forces FR and FL due to the bending stresses to the left and to the right of the beam. These forces will be resisted by the shearing force fvb dx acting at the boundary surface between the shaded and the unshaded portions.
For equilibrium of the upper shaded portion
FL+FV−FR=0
FV=FR−FL
Where
FV=fvbdx
FL=∫fb1dA;fb1=MyI
FR=∫fb2dA;fb2=(M+dM)yI
Fv=∫(M+dM)yIdA−∫MyIdA
fvbdx=∫MyIdA+∫dMIydA−∫MyI
fvbdx=dMI∫ydA
fv=1IbdMdx∫ydA
But dMdx=V, where V represents the shear at the section in N, and ∫ydA=Ay¯ represents the first moment of an area of the shaded section about N.A. in mm3 which we will denote as Q, then
fv=VQIb