TY - JOUR
T1 - Numerical models of salt diapir formation by down-building
T2 - The role of sedimentation rate, viscosity contrast, initial amplitude and wavelength
AU - Fuchs, L.
AU - Schmeling, H.
AU - Koyi, H.
PY - 2011/8
Y1 - 2011/8
N2 - Formation of salt diapirs has been described to be due to upbuilding (i.e. Rayleigh-Taylor like instability of salt diapirs piercing through a denser sedimentary overburden) or syndepositional down-building process (i.e. the top of the salt diapir remains at the surface all the time). Here we systematically analyse this second end-member mechanism by numerical modelling. Four parameters are varied: sedimentation ratevsed, salt viscosity ηsalt, amplitude δ of the initial perturbation of the sedimentation layer and the wavenumberkof this perturbation. The shape of the resulting salt diapirs strongly depends on these parameters. Small diapirs with subvertical side walls are found for small values ofvsed and ηsalt or large values of δ, whereas taller diapirs with pronounced narrow stems build for larges values ofvsed and ηsalt or small values of δ. Two domains are identified in the four-parameter space, which separates successful down-building models from non-successful models. By applying a simple channel flow law, the domain boundary can be described by the non-dimensional law, where is the sediment density scaled by the density contrast Δρ between sediment and salt, the wavelength is scaled by the salt layer thicknesshsalt, and velocity is scaled by ηsalt/(Δρg), where ηsalt is the salt viscosity andgis the gravitational acceleration. From the numerical models, the constantsC1 andC2 are determined as 0.0283 and 0.1171, respectively.
AB - Formation of salt diapirs has been described to be due to upbuilding (i.e. Rayleigh-Taylor like instability of salt diapirs piercing through a denser sedimentary overburden) or syndepositional down-building process (i.e. the top of the salt diapir remains at the surface all the time). Here we systematically analyse this second end-member mechanism by numerical modelling. Four parameters are varied: sedimentation ratevsed, salt viscosity ηsalt, amplitude δ of the initial perturbation of the sedimentation layer and the wavenumberkof this perturbation. The shape of the resulting salt diapirs strongly depends on these parameters. Small diapirs with subvertical side walls are found for small values ofvsed and ηsalt or large values of δ, whereas taller diapirs with pronounced narrow stems build for larges values ofvsed and ηsalt or small values of δ. Two domains are identified in the four-parameter space, which separates successful down-building models from non-successful models. By applying a simple channel flow law, the domain boundary can be described by the non-dimensional law, where is the sediment density scaled by the density contrast Δρ between sediment and salt, the wavelength is scaled by the salt layer thicknesshsalt, and velocity is scaled by ηsalt/(Δρg), where ηsalt is the salt viscosity andgis the gravitational acceleration. From the numerical models, the constantsC1 andC2 are determined as 0.0283 and 0.1171, respectively.
KW - Diapir and diapirism
KW - Mechanics, theory, and modelling
KW - Numerical solutions
KW - Sedimentary basin processes
UR - https://www.scopus.com/pages/publications/79960242177
U2 - 10.1111/j.1365-246X.2011.05058.x
DO - 10.1111/j.1365-246X.2011.05058.x
M3 - Article
AN - SCOPUS:79960242177
SN - 0956-540X
VL - 186
SP - 390
EP - 400
JO - Geophysical Journal International
JF - Geophysical Journal International
IS - 2
ER -