22 CHAPTER 1. PROPERTIES OF MATTER
P x
Q
A
B
C
φ
θ
dx
r
l
Fixed End
Free End
(twisted)
Figure 1.21: Couple per unit twist
The 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
n
x◊
l
B
◊(2fixdx)=
2 fin◊x^2
l
dx (1.9)
The torque about the axisPQacting on the shell is
(Force)◊(Distance) =
A
2 fin◊x^2
l
dx
B
◊x=
2 fin◊x^3
l
dx (1.10)