In Intr trod oducing ucing GA GAIA IA, th the bran e brand d - - PowerPoint PPT Presentation

in intr trod oducing ucing ga gaia ia th the bran e brand
SMART_READER_LITE
LIVE PREVIEW

In Intr trod oducing ucing GA GAIA IA, th the bran e brand d - - PowerPoint PPT Presentation

In Intr trod oducing ucing GA GAIA IA, th the bran e brand d new ew se sedi diment ment tr tran ansp spor ort t mod odule ule of th f the e TE TELE LEMA MAC-MAS MASCARE CARET T sy system stem Cont ntribut ributors


slide-1
SLIDE 1

In Intr trod

  • ducing

ucing GA GAIA IA, th the bran e brand d new ew se sedi diment ment tr tran ansp spor

  • rt

t mod

  • dule

ule of th f the e TE TELE LEMA MAC-MAS MASCARE CARET T sy system stem

Cont ntribut ributors to Gaia ia in alphab phabetica tical orde rder: : Yoann ann Audou

  • uin

in, , Th Thomas mas Bens nson,

  • n, Matthieu

thieu Deli linar nares, s, Jacqu ques es Fonta ntaine, ine, Boris ris Gland ander, Nicolas

  • las Huybr

ybrechts chts, , Rebekk bekka a Kopman ann, n, Agnès nès Ler eroy

  • y,

, Sar ara a Pav avan an, , Chi-Tuâ uân Pham, am, Flor

  • rent

nt Tacco cone, , Pabl ablo

  • Tassi

ssi & & Regi gis s Walthe alther r TU TUC 2019, 019, Cer erfa facs cs, , Toulou

  • use

se, , France rance

slide-2
SLIDE 2

GAIA is the new sedim iment ent transpo nsport t and bed evo voluti lution n modul ule e of the TMS

  • Developed for more than 25 years [Latteux & Tanguy, 1990]
  • Originally based on the same finite element structure as the 2D code solving the shallow water

equations, later baptized TELEMAC-2D

It’s based on the historical rical sedi diment ment transpo nsport t module ule SISY SYPHE PHE

  • Improvement of the trea

eatm tment ent of graded aded and nd mixed ed sedi dimen ments ts (cohesive and non-cohesive)

  • Full

ll compatib tibility ility betw twee een 2D and nd 3D proc

  • cesses

sses

  • Bett

tter disti tinction nction between sedimentary processes in the wat ater er column umn, , in the bed bed and d in the e water-be bed inter terfa face ce

  • Code optimization, error detections and corrections, etc.

Macro ideas behind GAIA’s developments

slide-3
SLIDE 3

Photos hackathons

slide-4
SLIDE 4
slide-5
SLIDE 5
slide-6
SLIDE 6
slide-7
SLIDE 7

Main n sediment ment transpo nsport t mech chan anis isms s in GAIA

  • IV. Bed evolution

(solved by Gaia)

slide-8
SLIDE 8
  • I. Sedim

iment ent transpo nsport t proce cess sses s in the water er co colum umn

  • IV. Bed evolution

(solved by Gaia)

slide-9
SLIDE 9
  • I. Sedim

iment ent transpo nsport t proce cess sses s in the water er co colum umn

Based on the solution of the equation describing the mass cons nser ervation ation of suspe pended nded sedim diment ent This advection-diffusion equation, with appropriate IC and BC, is solved ed by TELE LEMA MAC-2D 2D or TELE LEMA MAC-3D 3D

  • To stay up-to-date with the numer

merical cal sche hemes mes and d algorithm gorithm developments elopments in the hydr ydrod

  • dynamic

ynamics module ule for the solution of the advection terms

  • Clea

earer er disti tincti nction

  • n between sediment transport processes happening in the water colum

umn, e.g. sediment transport over a rigid bed

Suspended sediment particles being transported by the flow, maintaine tained d in suspe pension nsion above

  • ve the bot
  • ttom
  • m by the action

tion of upwar ard-mov moving ing turbule rbulent nt eddies dies

slide-10
SLIDE 10
  • IV. Bed evolution

(solved by Gaia)

II. . Sedim iment ent transp anspor

  • rt

t proce cess sses es in the bed and strati ratigrap graphy hy

slide-11
SLIDE 11

II. . Sedim iment ent transp anspor

  • rt

t proce cess sses es in the bed and strati ratigrap graphy hy

  • A. Bedlo

dload ad transpo ansport Sediment particles which are transported in direc ect t contact ntact with th the bott ttom or next to to the bed bed without being affected by the fluid turbulence In contrast to SISYPHE, in GAIA bedlo dload ad fluxes es are comput puted ed in ter terms of (dry) y) mass transpor nsport t rate per r unit width dth, , witho thout ut pores es: This is appr proach ach minimizes izes roundo ndoff ff error

  • rs, particularly for the mass transfer algorithms

used for the bed layer model

slide-12
SLIDE 12

II. . Sedim iment ent transp anspor

  • rt

t proce cess sses es in the bed and strati ratigrap graphy hy

B.

  • B. Bott

ttom

  • m strati

atigrap graphy hy

For sand graded distributions (gravel + sand), an algorithm bas ased ed on the e clas assi sical cal activ ive e layer er formul rmulation ation of Hira rano no is used [Blom, 2008] The bed model can be discr cretiz etized ed by a constant nstant numbe ber of layer ers along ng the e ve vertic tical l direc ectio tion, , allow

  • wed to

to be be empti tied ed during ring a simula latio tion The active layer suppl pplies ies mater terial ial that at can can be be erode

  • ded or
  • r depos

posit ited ed as bedload or suspended load

active layer

slide-13
SLIDE 13

II. . Sedim iment ent transp anspor

  • rt

t proce cess sses es in the bed and strati ratigrap graphy hy

  • C. Mixed

ed sedim iments ents

The bed model algorithm has been modified to to accou

  • unt

nt for r the e presence esence of mud or

  • r sand

and-mud mud mixtur ures The layer thickness results from the ma mass ss rati tio

  • of cohes

hesive and d non-coh cohesiv esive sedi diment ent

  • D. Consolidat

solidation ion

Based on the semi-empirical formulation originally developed by Villaret and Walther (2008), which ch uses es the iso-py pycnal cnal and nd first st-order der kinetics netics for

  • rmulati

ulations

  • ns

The presence of non-cohesive sediment in the stratigraphy doesn’t alter er the e sedim diment ent conso nsolida idatio tion

= +

< 40% % => > 40% % =>

+

slide-14
SLIDE 14
  • IV. Bed evolution

(solved by Gaia)

III II. . Sedim iment ent exch xchanges anges at the water er-bed bed inter erface face

slide-15
SLIDE 15

III II. . Sedim iment ent exch xchanges anges at the water er-bed bed inter erface face

The unified framework in 2D and 3D eliminat minates es unnece necessa ssary code de dupl plicati ication

  • n to compute the erosion
  • sion rat

ate E In GAIA, the e sedim diment ent depos positi tion

  • n tak

akes es place ce at all times mes rega egardless dless of the e value ue of the e bott ttom

  • m shear

hear stress ss, approach known as « simultaneous paradigm » [Winterwerp et al., 2012]

= +

> 50% % => E, t for cohes hesiv ive sedim diment ent < 30% % => E, t for non-co cohe hesiv sive sedim diment ent > 30% % and d < 50 50% % => E, t interpolat erpolated ed The composition

  • sition of the sedi

diment ment mixtur ture e in the surface (active) layer is considered when computing the critical shear stress for erosion t and the erosion rate E [Le Hir et al., 2011]

slide-16
SLIDE 16
  • IV. Bed evolution

(solved by Gaia)

IV. . Bed evo voluti lution

  • n
slide-17
SLIDE 17

IV. . Bed evo voluti lution

  • n

In GAIA, the bed evolution is computed by solving the mass ss conse nservatio tion equa uation ion for r sedi dimen ment or Exner equation, expr pres esse sed in term terms of mass: ss: Bedload, suspension or both sediment transport modes can can be be conside sidered ed simul ulta tane neous

  • usly

Two different morphological accelerators are proposed:

  • One accelerator suitable for river

er appl plications ications acco counting unting for r bedlo dload

  • One accelerator suitable for coast

astal al and d estua tuarine ne applic plicatio tions, as it is compatible with suspende spended sedim diment ent tran anspor sport Key physically-based processes that are retained in GAIA from SISYPHE include seco condar dary curr rrents ents, , bed bed slope pe effects fects, , bed bed roug ughne hness ss estim imat ator

  • rs,

, etc. c.

slide-18
SLIDE 18

Selected lected (new) keywor words ds from GAIA

CLASSES TYPE OF SEDIMENT = NCO;NCO;NCO;NCO;CO;CO;CO;CO CLASSES SEDIMENT DIAMETERS = 0.0002;0.0002;0.0002;0.0002;0.00001; 0.00001;0.00001;0.00001 CLASSES SETTLING VELOCITIES = -9.;-9.;-9.;-9.;0.001;0.001;0.001;0.001 /---------------------------------------------- BED LOAD FOR ALL SANDS = YES BED-LOAD TRANSPORT FORMULA FOR ALL SANDS = 5 SUSPENSION FOR ALL SANDS = YES SUSPENSION TRANSPORT FORMULA FOR ALL SANDS = 1 /---------------------------------------------- BED MODEL = 2 NUMBER OF LAYERS FOR INITIAL STRATIFICATION = 4 LAYERS INITIAL THICKNESS = 0.25;0.25;0.25;0.25 CLASSES INITIAL FRACTION = 0.15D0;0.15D0;0.15D0;0.15D0;0.1D0;0.1D0;0.1D0;0.1D0

> converter.py sis2gaia sis_cas gaia_cas

e.g. mixed sediment 4 c clas asses ses of non-cohe cohesi sive sedimen iments ts and 4 c clas asses ses of cohesiv esive sedimen ments ts; bed bed model el discr creti etized ed with th 4 4 laye yers, , accountin

  • unting for consol

solidation idation proces cesses ses

slide-19
SLIDE 19

Rh Rhine ne river ver applicatio lication n (GAIA vs vs SISY SYPHE PHE)

slide-20
SLIDE 20

Bott ttom evo voluti lution

  • n after

ter 6. 6.5 5 ye year ars

GAIA SISYPHE PHE D

slide-21
SLIDE 21

Mean diam amet eter er after ter 6. 6.5 5 ye years

GAIA SISYPHE PHE

slide-22
SLIDE 22

Ou Outlo look

Read ady-to to-use use, but still in progress… Do Docu cumentation ntation and V&V &V in progress ess (paper TUC 2019 intended as a mini-doc) The implementation of the Continuous Vertical grain Sorting Model CVSM is underway Please ase star art t us using ng GAI AIA A and post bug ugs, s, requests uests, sug uggest estio ions, ns, etc.

  • c. in the Forum

um

slide-23
SLIDE 23

Than Thank y k you

  • u

Gaea the Earth, Athenian red-figure calyx krater C5th B.C., Virginia Museum of Fine Arts