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Simulation of convection at a vertical ice face dissolving into saline water
by
Gayen, Bishakhdatta
, Kerr, Ross C.
, Griffiths, Ross W.
in
Ablation
/ Ambient temperature
/ Boundary layer
/ Boundary layer flow
/ Boundary layers
/ Buoyancy
/ Buoyancy flux
/ Convection
/ Convective flow
/ Diffusion
/ Diffusion rate
/ Direct numerical simulation
/ Dissolution
/ Dissolving
/ Drag
/ Drag coefficient
/ Drag coefficients
/ Dye dispersion
/ Dynamics
/ Experiments
/ Fluids
/ Freezing
/ Freezing point
/ Grashof number
/ Gravitational waves
/ Heat
/ Ice
/ Ice-water interface
/ Laboratories
/ Liquidus
/ Mathematical models
/ Melting points
/ Momentum
/ Mud-water interfaces
/ Saline water
/ Salinity
/ Seawater
/ Shear
/ Simulation
/ Temperature
/ Turbulence
/ Turbulent flow
/ Velocity
/ Water circulation
/ Water column
/ Water depth
/ Water temperature
2016
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Simulation of convection at a vertical ice face dissolving into saline water
by
Gayen, Bishakhdatta
, Kerr, Ross C.
, Griffiths, Ross W.
in
Ablation
/ Ambient temperature
/ Boundary layer
/ Boundary layer flow
/ Boundary layers
/ Buoyancy
/ Buoyancy flux
/ Convection
/ Convective flow
/ Diffusion
/ Diffusion rate
/ Direct numerical simulation
/ Dissolution
/ Dissolving
/ Drag
/ Drag coefficient
/ Drag coefficients
/ Dye dispersion
/ Dynamics
/ Experiments
/ Fluids
/ Freezing
/ Freezing point
/ Grashof number
/ Gravitational waves
/ Heat
/ Ice
/ Ice-water interface
/ Laboratories
/ Liquidus
/ Mathematical models
/ Melting points
/ Momentum
/ Mud-water interfaces
/ Saline water
/ Salinity
/ Seawater
/ Shear
/ Simulation
/ Temperature
/ Turbulence
/ Turbulent flow
/ Velocity
/ Water circulation
/ Water column
/ Water depth
/ Water temperature
2016
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Do you wish to request the book?
Simulation of convection at a vertical ice face dissolving into saline water
by
Gayen, Bishakhdatta
, Kerr, Ross C.
, Griffiths, Ross W.
in
Ablation
/ Ambient temperature
/ Boundary layer
/ Boundary layer flow
/ Boundary layers
/ Buoyancy
/ Buoyancy flux
/ Convection
/ Convective flow
/ Diffusion
/ Diffusion rate
/ Direct numerical simulation
/ Dissolution
/ Dissolving
/ Drag
/ Drag coefficient
/ Drag coefficients
/ Dye dispersion
/ Dynamics
/ Experiments
/ Fluids
/ Freezing
/ Freezing point
/ Grashof number
/ Gravitational waves
/ Heat
/ Ice
/ Ice-water interface
/ Laboratories
/ Liquidus
/ Mathematical models
/ Melting points
/ Momentum
/ Mud-water interfaces
/ Saline water
/ Salinity
/ Seawater
/ Shear
/ Simulation
/ Temperature
/ Turbulence
/ Turbulent flow
/ Velocity
/ Water circulation
/ Water column
/ Water depth
/ Water temperature
2016
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Simulation of convection at a vertical ice face dissolving into saline water
Journal Article
Simulation of convection at a vertical ice face dissolving into saline water
2016
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Overview
We investigate the convection and dissolution rate generated when a wall of ice dissolves into seawater under Antarctic Ocean conditions. In direct numerical simulations three coupled interface equations are used to solve for interface temperature, salinity and ablation velocity, along with the boundary layer flow and transport. The main focus is on ambient water temperatures between
$-1\\,^{\\circ }\\text{C}$
and
$6\\,^{\\circ }\\text{C}$
and salinities around 35 ‰, where diffusion of salt to the ice–water interface depresses the freezing point and enhances heat diffusion to the ice. We show that fluxes of both heat and salt to the interface are significant in governing the dissolution of ice, and the ablation velocity agrees well with experiments and a recent theoretical prediction. The same turbulent flow dynamics and ablation rate are expected to apply at any depth in a deeper ocean water column (after choosing the relevant pressure coefficient for the liquidus temperature). At Grashof numbers currently accessible by direct numerical simulation, turbulence is generated both directly from buoyancy flux and from shear production in the buoyancy-driven boundary layer flow, whereas shear production by the convective flow is expected to be more important at geophysical scales. The momentum balance in the boundary layer is dominated by buoyancy forcing and wall stress, with the latter characterised by a large drag coefficient.
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