Aim:
To determine the rigidity modulus of the material of a given cylindrical rod through telescope and scale method.
Apparatus:
Searle's static torsion apparatus: rod with attached pulley, weight hanger, slotted weights, telescope, mirror and scale.
Theory:
Shear modulus, or rigidity modulus n is defined as the ratio of stress F/A to strain ÃŽâ€Âx/l when a shearing force F is applied to a rigid block of height l and area A. ÃŽâ€Âx is the deformation of the block, and
(1) 
This is similar to what happens when a torque Ä is applied to a rigid rod of length l and radius r. Looking at the cross-section of the rod, consider a ring of width dr' at radius r' , which will have area 2Àr'dr', with force applied tangentially. The weighted average force over the cross-sectional area A of the rod is then
(2)
If the torque deforms the rod by twisting it through a small angle θ, the deformation distance (corresponding to ÃŽâ€Âx) at the outside edge of the rod is approximately θr. The definition of the rigidity modulus n becomes 
(3)
In our apparatus the torque Ä is supplied by hanging a weight of mass M from a string wound round a pulley of radius R, so Ä =MgR and our definition of rigidity modulus n becomes
(4)

Now suppose we mount a small mirror on the rod at distance l from its fixed end, and look at a centimeter scale in the mirror through an adjacent telescope, both at distance D from the mirror. When the rod deforms and the mirror rotates through a small angle θ , we look at a point on the scale a distance approximately S=2Dθ from the original point, which was aligned with the telescope. We can measure D and S and substitute θ =S/2D in our definition of rigidity modulus n, to get
(5)
Application:
Engineers consider the value of shear modulus when selecting materials for shafts, which are rods that are subjected to twisting torques.