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Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018

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Page 1: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA

Glacier Hydrology II: Theory and Modeling

Matt HoffmanGwenn Flowers, Simon Fraser

McCarthy Summer School 2018

Page 2: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Observations

6/13/18 | 2Los Alamos National Laboratory

Theory

Modeling

Page 3: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Governing equations for subglacial drainage

6/13/18 | 3Los Alamos National Laboratory

Continuity

Source/sinks

Fluid potential

Water flux

Evolution equation for element(s)

Gwenn Flowers

Page 4: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Conservation of mass (continuity) in a 1-D water sheet or film

6/13/18 | 4Los Alamos National Laboratory

Gwenn Flowers

Page 5: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Water sources, sinks, and fluxes

6/13/18 | 5Los Alamos National Laboratory

Page 6: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Governing equations for subglacial drainage

6/13/18 | 6Los Alamos National Laboratory

Continuity

Source/sinks

Fluid potential

Water flux

Evolution equation for element(s)

Gwenn Flowers

Page 7: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Laminar and turbulent flow

6/13/18 | 7Los Alamos National Laboratory

Navier-Stokes equationsfrom Conservation of Momentum for motion of fluids(Newton’s Second Law)

Inertialforces

Pressureforces

Viscousforces

Externalforces

Reynolds number:Used to predict laminar and turbulent flow regimes

InertialforcesViscousforces

Low Re

High Re

Page 8: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Laminar flow in sheet or film

6/13/18 | 8Los Alamos National Laboratory

Navier-Stokes equationfrom Conservation of Momentum

(Newton’s Second Law)

Here assuming:

• Incompressible

• Laminar

• Parallel shear flow

μ = Dynamic

viscosity of water

ρw = Density of water

v = water velocity

Φ = hydraulic potential

Inertial

forces

Pressure

forces

Viscous

forces

External

forces

Poiseuille FlowAssumptions:

• Steady-state

• Horizontal

• 1-d

Viscous

forces

Pressure

forces

Solve for velocity• Integrate twice

• Apply appropriate boundary

conditions

Solve for flux• Integrate velocity with depth

• Apply appropriate boundary

conditions

Solve for depth-averaged velocity

Laminar flow: q∝

pw

hh

Page 9: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Laminar flow in pipe or channel

6/13/18 | 9Los Alamos National Laboratory

Navier-Stokes equationRadial coordinates

Solve for velocity• Integrate twice• Apply appropriate boundary

conditions

Page 10: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Porous media flow: Darcy’s Law

6/13/18 | 10Los Alamos National Laboratory

Porous media flow• Creeping, laminar flow• Tortuous paths• Quantity of interest is not fluid

velocity but effective velocity

Hydraulic conductivityFlux Hydropotential

gradient

layerthickness

Relevant to:• Uneven water films • Bulk behavior of

linked cavity system (“microporous sheet”)

• Till canals• Nye channels• Drainage through till

Ian Hewitt

Page 11: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Turbulent flow in pipe or channel

6/13/18 | 11Los Alamos National Laboratory

• Can be derived from Navier-Stokes equations• More intuitive: balance of driving pressure

force and resistive viscous force

Potential gradient

Area Perimeter Wall stress

Wall stress:Empirical from engineering hydraulics• Darcy-Weisbach• Gauckler-Manning-

Strickler

Frictionfactor

Combine to solve for velocity: Turbulent flow: q∝

1/2

Page 12: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Governing equations for subglacial drainage

6/13/18 | 12Los Alamos National Laboratory

Continuity

Source/sinks

Fluid potential

Water flux

Evolution equation for element(s)

Gwenn Flowers

Page 13: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Energy balance for melt:

Model output: sheet thickness, water pressure

Meltopening

Slidingover

bumps

Creep closure of ice

v

v

ice

bed

Modified from Anderson, et al. 2004

Evolution of conduit (channel or cavity) volume

ConduitEvolution:

Geothermalheat flux

Frictionalheating

Viscousdissipation

(laminar or turbulent)

Page 14: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Melt opening of a channel

6/13/18 | 14Los Alamos National Laboratory

Viscous dissipation• power per unit length of conduit• release of potential energy

(gravitational + pressure)

Pressure-melt dependence• when pressure varies• some power required to keep water

at melt temperature

Pressuremeltingcoefficent

Specificheat capacityof water

~0.3

Net power

As a melt rate• Instantaneous heat transfer• Temperate ice• More complex treatment

using full energy balance

Page 15: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Creep closure for a channel

6/13/18 | 15Los Alamos National Laboratory

Glen’s flow law• Radial coordinates

Rewrite as area change

Complexities• Conduit shape – channels can be low and broad, non-channel shapes

• Addition of shape factor• Effective pressure typically substituted for normal stress

Page 16: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Classic conduit evolution mechanisms

6/13/18 | 16Los Alamos National Laboratory

Channelized DrainageImage: Tim CreytsImage: Ian Hewitt

Distributed Drainage

Opening

Closing

Sliding

Melting

Creep

YES(but other mechanisms also possible)

Passive sources

Viscous dissipation

Yes(but other mechanisms also possible)

Yes

No/not important(but maybe can destroy)

Maybe No/not important

No(can lead to channelization)

YES(can also cause closing)

Page 17: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Classic conduit evolution mechanisms

6/13/18 | 17Los Alamos National Laboratory

Channelized DrainageImage: Tim CreytsImage: Ian Hewitt

Distributed Drainage

Energy balance for melt:

Meltopening

Slidingover

bumps

Creep closure of

ice

ConduitEvolution:

Geothermalheat flux

Frictionalheating

Viscousdissipation

(laminar or turbulent)

Meltopening

Slidingover

bumps

Creep closure of

ice

Geothermalheat flux

Frictionalheating

Viscousdissipation

(laminar or turbulent)

Page 18: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Governing equations for subglacial drainage

6/13/18 | 18Los Alamos National Laboratory

Continuity

Source/sinks

Fluid potential

Water flux

Evolution equation for element(s)

Gwenn Flowers

Page 19: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 19Los Alamos National Laboratory

Putting it together: implications

Gwenn Flowers

Page 20: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Implications: channel vs. distributed drainage efficiency

6/13/18 | 20Los Alamos National Laboratory

channel

distributed

Page 21: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Observations

6/13/18 | 21Los Alamos National Laboratory

Theory

Modeling

Page 22: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Literature: models of subglacial drainage

6/13/18 | 22Los Alamos National Laboratory

Gwenn Flowers

Page 23: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Overview: models of subglacial drainage

6/13/18 | 23Los Alamos National Laboratory

Gwenn Flowers

Page 24: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 24Los Alamos National Laboratory

Elements of the subglacial drainage system

Page 25: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Elements of the subglacial drainage system

6/13/18 | 25Los Alamos National Laboratory

Page 26: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Overview: Models of subglacial drainage

6/13/18 | 26Los Alamos National Laboratory

Flowers (2015) Proc. Royal Soc. A

Page 27: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Recipe for a model of subglacial drainage

6/13/18 | 27Los Alamos National Laboratory

Gwenn Flowers

Page 28: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Early models from groundwater hydrology (1970s – 1990s)

6/13/18 | 28Los Alamos National Laboratory

Gwenn Flowers

Page 29: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 29Los Alamos National Laboratory

Gwenn Flowers

Page 30: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 30Los Alamos National Laboratory

Page 31: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 31Los Alamos National Laboratory

• Motivated by an interest in basal till deformation, fast flow, fate of basal melt, impact of glaciation on groundwater

• Hydrogeologic units beneath ice sheets rarely capable of evacuating even basal melt from ice sheets

• Some interfacial drainage system required, though rarely formalized

Gwenn Flowers

Page 32: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 32Los Alamos National Laboratory

Gwenn Flowers

Page 33: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 33Los Alamos National Laboratory

Focus on drainage at the ice-bed interfaceModels employ more of the theoretical drainage elements

“Next-generation” glaciological models (1990s ±)

Gwenn Flowers

Page 34: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 34Los Alamos National Laboratory

Gwenn Flowers

Page 35: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 35Los Alamos National Laboratory

Page 36: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 36Los Alamos National Laboratory

Page 37: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 37Los Alamos National Laboratory

Gwenn Flowers

Page 38: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Integrating multiple drainage elements (2000s – present)

6/13/18 | 38Los Alamos National Laboratory

Gwenn Flowers

Page 39: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 39Los Alamos National Laboratory

Gwenn Flowers

Page 40: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 40Los Alamos National Laboratory

Gwenn Flowers

Page 41: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 41Los Alamos National Laboratory

Page 42: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 42Los Alamos National Laboratory

Page 43: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 43Los Alamos National Laboratory

Page 44: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 44Los Alamos National Laboratory

Page 45: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 45Los Alamos National Laboratory

Page 46: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 46Los Alamos National Laboratory

Subglacial drainage model zoo

Subglacial Hydrology Model Intercomparison Project (SHMIP)de Fleurian et al. in review, J. Glac.

Page 47: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 47Los Alamos National Laboratory

Features of current models

• Correct (?) physics applied to fast and slow drainage systems

• Numerical formulation (2D distributed system, network of 1D channel

elements)

• Dynamic evolution of drainage system

• Two-way coupling to sliding/friction laws

Modelling challenges and limitations

• Resolution of individual channel elements

• Assumption of fully “connected” drainage system

• Temperate bed assumption

• Dearth of calibration/validation data, resolution of input data

Page 48: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 48Los Alamos National Laboratory

Gwenn Flowers

Page 49: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 49Los Alamos National Laboratory

Field observations more complex and richer than current models can explain• Out of phase borehole pressure variations• Water pressure above floatation pressure• Large pressure gradients between neighboring

boreholes• Switching between “connected” and “disconnected”

behavior• Very high winter water pressure despite negligible

water input• …

Too simple?

Rada and Schoof (2018) Subglacial drainage characterization from eight years of continuous borehole data on a small glacier in the Yukon Territory, Canada. The Cryosphere Discussions.

Page 50: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 50Los Alamos National Laboratory

Downs, J. Z., et al. (2018) Dynamic hydraulic conductivity reconciles mismatch between modeled and observed winter subglacial water pressure, J. Geophys. Res. Earth Surf., 123, 818–836.

Summer Winter Summer Winter

Page 51: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 51Los Alamos National Laboratory

Hoffman, et al. (2016) Greenland subglacial drainage evolution regulated by weakly-connected

regions of the bed, Nat. Commun., 7, 13903.

Page 52: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 52Los Alamos National Laboratory

Spring

Summer

Fall

Hoffman, et al. (2016) Greenland subglacial drainage evolution regulated by weakly-connected

regions of the bed, Nat. Commun., 7, 13903.

Iken, A., and M. Truffer (1997), The relationship between

subglacial water pressure and velocity of

Findelengletscher, Switzerland, during its advance and

retreat, J. Glaciol., 43(144), 328–338.

Ice dynamics responds to integrated

basal traction over entire bed.

Page 53: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

6/13/18 | 53Los Alamos National Laboratory

Rada and Schoof (2018) Subglacial drainage characterization from eight years of continuous borehole data on a small glacier in the Yukon

Territory, Canada. The Cryosphere Discussions.

Page 54: Glacier Hydrology II: Theory and Modeling · Glacier Hydrology II: Theory and Modeling Matt Hoffman Gwenn Flowers, Simon Fraser McCarthy Summer School 2018. Observations Los Alamos

Recommendations for ongoing and future work

6/13/18 | 54Los Alamos National Laboratory

• Efficient representation of drainage networks in large-

scale models

• Continuum approached for efficient drainage that

converge with grid resolution

• Alternative approaches to continuum models or explicit

treatment of “connected” and “unconnected” bed areas

• Unified treatment of hard and soft beds?

• More attention to polythermal conditions (c.f. e.g. Bueler

and Brown, 2009; Creyts and Clarke, 2010)

• Surface, englacial, groundwater drainage

• Develop methods to “measure” basal water pressure at

scales commensurate with ice dynamics