22 CHAPTER 1. PROPERTIES OF MATTER
P xQABCφθdxr
l
Fixed EndFree End
(twisted)Figure 1.21: Couple per unit twistThe Rigidity Modulus of the wire (n) = (shear stress) / (shear strain).
Hence, shear stress,=n◊(shear strain) (1.6)We first consider an imaginary cylindrical shell of outer radiusxand thicknessdxas
shown in Figure5.65and calculate the shear stress at this shell. A vertical line AB drawn
on the shell get shifted to the position AC due to the torsional deformation, resulting in
an angle of twist\BQC=◊and an angle of shear\BAC=„.Itcanbeseenfrom
Figure5.65thatBC=l„=x◊. Therefore,
shear strain,„=x◊
l(1.7)
Therefore from equations (5.281) and (5.282), at the imaginary shell,
shear stress,=n◊x◊
l(1.8)
The area of cross-section of the imaginary shell = circumference◊width =(2fix)◊(dx).
Therefore, force acting in the shell cross-section is
Force = (shear stress)◊(area) =A
nx◊
lB
◊(2fixdx)=2 fin◊x^2
ldx (1.9)The torque about the axisPQacting on the shell is
(Force)◊(Distance) =A
2 fin◊x^2
ldxB
◊x=2 fin◊x^3
ldx (1.10)