2021
DOI: 10.1016/j.tecto.2021.228870
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Normal fault reactivation during multiphase extension: Analogue models and application to the Turkana depression, East Africa

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Cited by 29 publications
(42 citation statements)
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“…We start with the basic formula addressing the stress ratios between model and nature (σ model /σ nature ) : σ * = ρ * × h * × g * , where ρ * , h * and g * are density, length and gravity ratios, respectively (Hubbert, 1937;Ramberg, 1981). We can then acquire the strain rate ratioε * from the stress and viscosity ratios σ * and η * (Weijermars and Schmeling, 1986):ε * = σ * /η * . Knowing the strain rate ratio, the following equations yield the velocity and time ratios (v * and t * ) :ε * = v/h * = 1/t * .…”
Section: Scalingmentioning
confidence: 99%
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“…We start with the basic formula addressing the stress ratios between model and nature (σ model /σ nature ) : σ * = ρ * × h * × g * , where ρ * , h * and g * are density, length and gravity ratios, respectively (Hubbert, 1937;Ramberg, 1981). We can then acquire the strain rate ratioε * from the stress and viscosity ratios σ * and η * (Weijermars and Schmeling, 1986):ε * = σ * /η * . Knowing the strain rate ratio, the following equations yield the velocity and time ratios (v * and t * ) :ε * = v/h * = 1/t * .…”
Section: Scalingmentioning
confidence: 99%
“…Handin, 1969;Jaeger and Cook, 1976;Twiss and Moore, 1992) but is acceptable, since in nature, the lithosphere is generally weakened by several phases of deformation. When assessing viscous materials, the Ramberg number R m applies (Weijermars and Schmeling, 1986): R m = gravitational stress / viscous strength = (ρ × g × h 2 )/(η × v). The Ramberg number for both the model and natural materials is 17.…”
Section: Scalingmentioning
confidence: 99%
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