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SHEAR MODULUS
In materials science, shear modulus, G, or sometimes S, sometimes referred to as the modulus of rigidity, is defined as the ratio of shear stress to the shear strain:

where F/A is shear stress and Δx/h is shear strain.
Shear modulus is usually measured in ksi (thousands of pounds per square inch) or GPa (gigapascals).
Typical values
The following are values of the shear modulus for select isotropic materials at room temperature:
| Material |
Shear modulus (GPa)[1] |
| Steel |
75.8 |
| Copper |
63.4 |
| Titanium |
41.4 |
| Glass |
26.2 |
| Aluminum |
25.5 |
| Polyethylene |
0.117 |
| Rubber |
0.0003 |
Explanation
The shear modulus is one of several quantities for measuring the strength of materials. All of them arise in the generalized Hooke's law. Young's modulus describes the material's response to linear strain (like pulling on the ends of a wire), the bulk modulus describes the material's response to uniform pressure, and the shear modulus describes the material's response to shearing strains. Anisotropic materials such as wood and paper exhibit differing material response to stress or strain when tested in different directions.
In solids, there are two kinds of sound waves, pressure waves and shear waves. The speed of sound for shear waves is controlled by the shear modulus.
See also
References
- ^ Crandall, Dahl, Lardner (1959). An Introduction to the Mechanics of Solids. McGraw-Hill.
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