Byerlee's law

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Byerlee's law is an experimentally derived law in physics that gives the stress circumstances in the Earth's crust at which fracturing along a geological fault takes place. The relation was determined by American geophysicist James Byerlee, by using experimental data to solve the Mohr–Coulomb failure criterion.[1]

Mohr-Coulombs criterion is a linear function of shear stress over normal stress, at the point of brittle failure inside a material:

\tau = S _0 + \mu (\sigma _n - P _f)

In which \tau is the shear stress and \sigma _n the normal stress. S _0 is the cohesion or internal strength of the material. The value P _f is the pore fluid pressure inside a rock, which is constant on a small scale and weakens the rock. Byerlee found that in the upper crust, the criterion can be simplified to:

 \tau = 0.85 \sigma _n

for normal stresses up to 200 MPa; and

 \tau = 50 + 0.6\sigma _n

for normal stresses higher than 200 MPa. In both formulas the shear stress is given in MPa.

However, the crust is far from a homogeneous material and consists of many rock types. Material constants can therefore vary locally. Even though Byerlee's law is a simplification, it is a good enough approximation for almost all situations. Byerlee's law gets less accurate when pressures and temperatures get higher than normal in the upper crust (e.g. temperatures over 400°C)

See also [edit]

References [edit]

  1. ^ Byerlee, J.D. (1978). "Friction of rocks". Pure and Applied Geophysics 116 (4–5): 615–626. Bibcode:1978PApGe.116..615B. doi:10.1007/BF00876528.