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Used Fuel Disposition Campaign
Next-Gen PA Model: Approach for
Colloid-Facilitated Transport
Paul Reimus and Mavrik Zavarin
Model Integration Session
UFD Working Group Meeting
June 8, 2016
Used
Fuel
Disposition
2
0.00001
0.0001
0.001
0.01
0.1
1
0 50 100 150 200
Concentration(C/Co)
Pore Volumes
Conservative RN
Retarded RN with No Colloids
CFT Kinetic Control
CFT Equilibrium Control
6/8/2016 CFT Lightning
Function of ([exp(-kdesฯ„) x exp(-kfiltฯ„)])
d
B
K1R
ฯ†
ฯ
+=
CK1
K1
CK1
CKK1
R
colcold,
d
B
colcold,
colcold,d
B
eff
+
+
โ‰ˆ
+
++
=
ฯ†
ฯ
ฯ†
ฯ
Two Transport Regimes โ€“ Easy to
Model, Difficult to Mechanistically
Parameterize
Used
Fuel
Disposition
Colloid Transport Equations
๏ฎ Colloid Transport (General):
๐๐๐‘ช๐‘ช๐’„๐’„
๐๐๐’•๐’•
+ ๐’…๐’…๐’…๐’… ๐’…๐’… ๐’—๐’—๐’„๐’„ ๐‘ช๐‘ช๐’„๐’„ + ๐‘ซ๐‘ซ๐’„๐’„ ๐›๐›๐‘ช๐‘ช๐’„๐’„ =
โˆ’๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡
๐‘บ๐‘บ๐‘บ๐‘บ
๐‘ฝ๐‘ฝ
๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘บ๐‘บ๐’„๐’„
๐‘บ๐‘บ๐’„๐’„,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž
+ ๐’Œ๐’Œ๐’“๐’“๐’“๐’“
๐‘บ๐‘บ๐‘บ๐‘บ
๐‘ฝ๐‘ฝ
๐‘บ๐‘บ๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š
๐‘บ๐‘บ๐‘บ๐‘บ
๐‘ฝ๐‘ฝ
๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž
+
๐‘บ๐‘บ๐‘บ๐‘บ
๐‘ฝ๐‘ฝ
๐‘ท๐‘ท๐’„๐’„
๐๐๐‘บ๐‘บ๐’„๐’„
๐๐๐’•๐’•
= ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘บ๐‘บ๐’„๐’„
๐‘บ๐‘บ๐’„๐’„,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž
โˆ’ ๐’Œ๐’Œ๐’“๐’“๐’“๐’“ ๐‘บ๐‘บ๐’„๐’„
๐๐๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
๐๐๐’•๐’•
= ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž
๏ฎ At a true steady state,
๐๐๐‘บ๐‘บ๐’„๐’„
๐๐๐’•๐’•
= ๐ŸŽ๐ŸŽ, ๐š๐š๐š๐š๐š๐š ๐‘ท๐‘ท๐’„๐’„ โ‰… ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž
3
Reversible Filtration Irreversible Filtration Production
Mobile Colloids
Reversibly Immobilized Colloids
Irreversibly Immobilized Colloids
6/8/2016 CFT Lightning
Assume colloids limited to flowing domain
Used
Fuel
Disposition
Solute Transport Equations
๏ฎ Mobile Solute Transport Equation:
๐๐๐‘ช๐‘ช๐’‚๐’‚
๐๐๐’•๐’•
+ ๐’…๐’…๐’…๐’… ๐’…๐’… ๐’—๐’—๐’‚๐’‚ ๐‘ช๐‘ช๐’‚๐’‚ + ๐‘ซ๐‘ซ๐’‚๐’‚ ๐›๐›๐‘ช๐‘ช๐’‚๐’‚ =
๏ฟฝ โˆ’๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š
๐†๐†๐‘ฉ๐‘ฉ
โˆ…
๐‘ช๐‘ช๐’‚๐’‚ ๐Ÿ๐Ÿ โˆ’
๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š
๐‘บ๐‘บ๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š
+ ๐’Œ๐’Œ๐’”๐’”๐’”๐’”,๐’Š๐’Š
๐†๐†๐‘ฉ๐‘ฉ
โˆ…
๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š
๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’
๐’Š๐’Š= ๐Ÿ๐Ÿ
+
๏ฟฝ โˆ’๐’Œ๐’Œ๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„
+ ๐’Œ๐’Œ๐’„๐’„๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„
๐’๐’๐’„๐’„๐’„๐’„๐’„๐’„๐’”๐’”๐’”๐’”๐’”๐’”๐’”๐’”๐’”๐’”
๐’Š๐’Š= ๐Ÿ๐Ÿ
+
๏ฟฝ
๐‘บ๐‘บ๐‘บ๐‘บ
๐‘ฝ๐‘ฝ
โˆ’๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘บ๐‘บ๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„
+ ๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐Ÿ๐Ÿ โˆ’
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’
๐’Š๐’Š= ๐Ÿ๐Ÿ
+ terms accounting for matrix diffusion or diffusion into secondary porosity
๏ฎ Solute Sorbed onto Immobile Surfaces (nsites equations):
๐๐๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š
๐๐๐’•๐’•
= ๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐Ÿ๐Ÿ โˆ’
๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š
๐‘บ๐‘บ๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š
โˆ’ ๐’Œ๐’Œ๐’”๐’”๐’”๐’”,๐’Š๐’Š ๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š
4
(Flowing domain only; more terms
needed if secondary porosity)
6/8/2016 CFT Lightning
Used
Fuel
Disposition
Solute Associated with Colloids
Equations
๏ฎ Solute Sorbed to Mobile Colloids (ncolsites equations):
๐๐๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„
๐๐๐’•๐’•
+ ๐’…๐’…๐’…๐’… ๐’…๐’… ๐’—๐’—๐’‚๐’‚ ๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ + ๐‘ซ๐‘ซ๐’„๐’„ ๐›๐›๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ = ๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„
โˆ’ ๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„
โˆ’๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡
๐‘บ๐‘บ๐‘บ๐‘บ
๐‘ฝ๐‘ฝ
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘บ๐‘บ๐’„๐’„
๐‘บ๐‘บ๐’„๐’„,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž
+ ๐’Œ๐’Œ๐’“๐’“๐’“๐’“
๐‘บ๐‘บ๐‘บ๐‘บ
๐‘ฝ๐‘ฝ
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š
๐‘บ๐‘บ๐‘บ๐‘บ
๐‘ฝ๐‘ฝ
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž
๏ฎ Solute Sorbed to Immobile Colloids (ncolsites equations):
๐๐๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„
๐๐๐’•๐’•
= ๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘บ๐‘บ๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„
โˆ’ ๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ +
๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐Ÿ๐Ÿ โˆ’
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
โˆ’ ๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
โˆ’๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„
+ ๐’Œ๐’Œ๐’“๐’“๐’“๐’“ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ ๐Ÿ๐Ÿ โˆ’
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š
56/8/2016 CFT Lightning
Used
Fuel
Disposition
Additional Solute Detail on Colloid
or Immobile Media Surfaces
๏ฎ Transformations on Surfaces (from Mavrik, with extensions/generalizations
from Paul):
6
Surface Mediated-Reduction
With โ€˜Agingโ€™ of Reduced
Surface Species
Ca
Sa,1
Sa,2
Aging Process Only
Ca
Sa,1 Sa,2
Ca
Two Sorption Sites
with Surface
Transformation
Surfaces could be Colloids or Immobile Media
6/8/2016 CFT Lightning
Used
Fuel
Disposition
Total Conservative Mass Fraction โ€“
A Simplification
๏ฎ โ€˜Convolutionโ€™ of fraction of nonfiltering colloids with fraction of
nondesorbing solutes
๏ฎ That is, โ€˜fraction of solute not desorbing from fraction of colloids not
filtering over transport time ฯ„ โ€™, given by:
= ๏ฟฝ ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ โˆ’
๐‘บ๐‘บ๐‘บ๐‘บ
๐‘ฝ๐‘ฝ
๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐‰๐‰ ๏ฟฝ ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ โˆ’๐’Œ๐’Œ๐’„๐’„๐’„๐’„ ๐‰๐‰ ๐‘ท๐‘ท ๐’Œ๐’Œ๐’„๐’„๐’„๐’„
๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž
๐ŸŽ๐ŸŽ
๐’…๐’…๐’Œ๐’Œ๐’„๐’„๐’„๐’„
๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡
๐‘ท๐‘ท ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡
๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž
๐ŸŽ๐ŸŽ
๐’…๐’…๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡
76/8/2016 CFT Lightning
Used
Fuel
Disposition
Other Simplifications
๏ฎ If the time scale of transport is long relative to both forward and reverse rates of
any given reaction, that reaction can be assumed to be at equilibrium
โ€“ Good rule of thumb is if (SA/V)kfฯ„ > 5-10 and krฯ„ > 5-10, then equilibrium assumption is good
โ€“ Also, if sorption/filtration site density (Smax) is very large, then linear Kd-type approach works
๏ฎ Every linear equilibrium assumption reduces number of equations by one
(sorbed or filtered species equation is eliminated)
๏ฎ Special case of all reactions being at equilibrium and having a steady-state
colloid concentration, Ccol :
8
0=+ 2
2
x
C
CKv
t
C
CK
t
C
K+
x
C
D
x
C
v
t
C
colcfcolcd
B
cf
โˆ‚
โˆ‚
+
โˆ‚
โˆ‚
+
โˆ‚
โˆ‚
โˆ‚
โˆ‚
โˆ’
โˆ‚
โˆ‚
โˆ‚
โˆ‚
ฯ†
ฯ
( ) 0=1+1 2
2
x
C
D
x
C
vCK
t
C
CKK cfcolccolcd
B
โˆ‚
โˆ‚
โˆ’
โˆ‚
โˆ‚
+
โˆ‚
โˆ‚
๏ฃท๏ฃท
๏ฃธ
๏ฃถ
๏ฃฌ๏ฃฌ
๏ฃญ
๏ฃซ
++
ฯ†
ฯ
colc
colcd
B
C
CK
CKK
R
+
++
=
1
1
ฯ†
ฯ
Solute Transport Eq.:
Rearranged:
Effective Solute Retardation Factor:
Note Kd = kas/ksa, Kc = kac/kca
6/8/2016 CFT Lightning

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  • 2. Used Fuel Disposition 2 0.00001 0.0001 0.001 0.01 0.1 1 0 50 100 150 200 Concentration(C/Co) Pore Volumes Conservative RN Retarded RN with No Colloids CFT Kinetic Control CFT Equilibrium Control 6/8/2016 CFT Lightning Function of ([exp(-kdesฯ„) x exp(-kfiltฯ„)]) d B K1R ฯ† ฯ += CK1 K1 CK1 CKK1 R colcold, d B colcold, colcold,d B eff + + โ‰ˆ + ++ = ฯ† ฯ ฯ† ฯ Two Transport Regimes โ€“ Easy to Model, Difficult to Mechanistically Parameterize
  • 3. Used Fuel Disposition Colloid Transport Equations ๏ฎ Colloid Transport (General): ๐๐๐‘ช๐‘ช๐’„๐’„ ๐๐๐’•๐’• + ๐’…๐’…๐’…๐’… ๐’…๐’… ๐’—๐’—๐’„๐’„ ๐‘ช๐‘ช๐’„๐’„ + ๐‘ซ๐‘ซ๐’„๐’„ ๐›๐›๐‘ช๐‘ช๐’„๐’„ = โˆ’๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐‘บ๐‘บ๐‘บ๐‘บ ๐‘ฝ๐‘ฝ ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘บ๐‘บ๐’„๐’„ ๐‘บ๐‘บ๐’„๐’„,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž + ๐’Œ๐’Œ๐’“๐’“๐’“๐’“ ๐‘บ๐‘บ๐‘บ๐‘บ ๐‘ฝ๐‘ฝ ๐‘บ๐‘บ๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š ๐‘บ๐‘บ๐‘บ๐‘บ ๐‘ฝ๐‘ฝ ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž + ๐‘บ๐‘บ๐‘บ๐‘บ ๐‘ฝ๐‘ฝ ๐‘ท๐‘ท๐’„๐’„ ๐๐๐‘บ๐‘บ๐’„๐’„ ๐๐๐’•๐’• = ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘บ๐‘บ๐’„๐’„ ๐‘บ๐‘บ๐’„๐’„,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž โˆ’ ๐’Œ๐’Œ๐’“๐’“๐’“๐’“ ๐‘บ๐‘บ๐’„๐’„ ๐๐๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐๐๐’•๐’• = ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž ๏ฎ At a true steady state, ๐๐๐‘บ๐‘บ๐’„๐’„ ๐๐๐’•๐’• = ๐ŸŽ๐ŸŽ, ๐š๐š๐š๐š๐š๐š ๐‘ท๐‘ท๐’„๐’„ โ‰… ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž 3 Reversible Filtration Irreversible Filtration Production Mobile Colloids Reversibly Immobilized Colloids Irreversibly Immobilized Colloids 6/8/2016 CFT Lightning Assume colloids limited to flowing domain
  • 4. Used Fuel Disposition Solute Transport Equations ๏ฎ Mobile Solute Transport Equation: ๐๐๐‘ช๐‘ช๐’‚๐’‚ ๐๐๐’•๐’• + ๐’…๐’…๐’…๐’… ๐’…๐’… ๐’—๐’—๐’‚๐’‚ ๐‘ช๐‘ช๐’‚๐’‚ + ๐‘ซ๐‘ซ๐’‚๐’‚ ๐›๐›๐‘ช๐‘ช๐’‚๐’‚ = ๏ฟฝ โˆ’๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐†๐†๐‘ฉ๐‘ฉ โˆ… ๐‘ช๐‘ช๐’‚๐’‚ ๐Ÿ๐Ÿ โˆ’ ๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š + ๐’Œ๐’Œ๐’”๐’”๐’”๐’”,๐’Š๐’Š ๐†๐†๐‘ฉ๐‘ฉ โˆ… ๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š ๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’ ๐’Š๐’Š= ๐Ÿ๐Ÿ + ๏ฟฝ โˆ’๐’Œ๐’Œ๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ + ๐’Œ๐’Œ๐’„๐’„๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐’๐’๐’„๐’„๐’„๐’„๐’„๐’„๐’”๐’”๐’”๐’”๐’”๐’”๐’”๐’”๐’”๐’” ๐’Š๐’Š= ๐Ÿ๐Ÿ + ๏ฟฝ ๐‘บ๐‘บ๐‘บ๐‘บ ๐‘ฝ๐‘ฝ โˆ’๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘บ๐‘บ๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ + ๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐Ÿ๐Ÿ โˆ’ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’๐’ ๐’Š๐’Š= ๐Ÿ๐Ÿ + terms accounting for matrix diffusion or diffusion into secondary porosity ๏ฎ Solute Sorbed onto Immobile Surfaces (nsites equations): ๐๐๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š ๐๐๐’•๐’• = ๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐Ÿ๐Ÿ โˆ’ ๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š โˆ’ ๐’Œ๐’Œ๐’”๐’”๐’”๐’”,๐’Š๐’Š ๐‘บ๐‘บ๐’‚๐’‚,๐’Š๐’Š 4 (Flowing domain only; more terms needed if secondary porosity) 6/8/2016 CFT Lightning
  • 5. Used Fuel Disposition Solute Associated with Colloids Equations ๏ฎ Solute Sorbed to Mobile Colloids (ncolsites equations): ๐๐๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐๐๐’•๐’• + ๐’…๐’…๐’…๐’… ๐’…๐’… ๐’—๐’—๐’‚๐’‚ ๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ + ๐‘ซ๐‘ซ๐’„๐’„ ๐›๐›๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ = ๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ โˆ’๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐‘บ๐‘บ๐‘บ๐‘บ ๐‘ฝ๐‘ฝ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘บ๐‘บ๐’„๐’„ ๐‘บ๐‘บ๐’„๐’„,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž + ๐’Œ๐’Œ๐’“๐’“๐’“๐’“ ๐‘บ๐‘บ๐‘บ๐‘บ ๐‘ฝ๐‘ฝ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š ๐‘บ๐‘บ๐‘บ๐‘บ ๐‘ฝ๐‘ฝ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž ๏ฎ Solute Sorbed to Immobile Colloids (ncolsites equations): ๐๐๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ ๐๐๐’•๐’• = ๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘บ๐‘บ๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ + ๐’Œ๐’Œ๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚ ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐Ÿ๐Ÿ โˆ’ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š โˆ’ ๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š โˆ’๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘ช๐‘ช๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ + ๐’Œ๐’Œ๐’“๐’“๐’“๐’“ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ โˆ’ ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Š๐’Š๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„ ๐Ÿ๐Ÿ โˆ’ ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š ๐‘ช๐‘ช๐’‚๐’‚๐’‚๐’‚,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž,๐’Š๐’Š ๐‘บ๐‘บ๐’„๐’„,๐’Š๐’Š๐’Š๐’Š 56/8/2016 CFT Lightning
  • 6. Used Fuel Disposition Additional Solute Detail on Colloid or Immobile Media Surfaces ๏ฎ Transformations on Surfaces (from Mavrik, with extensions/generalizations from Paul): 6 Surface Mediated-Reduction With โ€˜Agingโ€™ of Reduced Surface Species Ca Sa,1 Sa,2 Aging Process Only Ca Sa,1 Sa,2 Ca Two Sorption Sites with Surface Transformation Surfaces could be Colloids or Immobile Media 6/8/2016 CFT Lightning
  • 7. Used Fuel Disposition Total Conservative Mass Fraction โ€“ A Simplification ๏ฎ โ€˜Convolutionโ€™ of fraction of nonfiltering colloids with fraction of nondesorbing solutes ๏ฎ That is, โ€˜fraction of solute not desorbing from fraction of colloids not filtering over transport time ฯ„ โ€™, given by: = ๏ฟฝ ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ โˆ’ ๐‘บ๐‘บ๐‘บ๐‘บ ๐‘ฝ๐‘ฝ ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐‰๐‰ ๏ฟฝ ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ๐‘ฌ โˆ’๐’Œ๐’Œ๐’„๐’„๐’„๐’„ ๐‰๐‰ ๐‘ท๐‘ท ๐’Œ๐’Œ๐’„๐’„๐’„๐’„ ๐’Œ๐’Œ๐’„๐’„๐’„๐’„,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž ๐ŸŽ๐ŸŽ ๐’…๐’…๐’Œ๐’Œ๐’„๐’„๐’„๐’„ ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐‘ท๐‘ท ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ ๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡,๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž๐’Ž ๐ŸŽ๐ŸŽ ๐’…๐’…๐’Œ๐’Œ๐’‡๐’‡๐’‡๐’‡ 76/8/2016 CFT Lightning
  • 8. Used Fuel Disposition Other Simplifications ๏ฎ If the time scale of transport is long relative to both forward and reverse rates of any given reaction, that reaction can be assumed to be at equilibrium โ€“ Good rule of thumb is if (SA/V)kfฯ„ > 5-10 and krฯ„ > 5-10, then equilibrium assumption is good โ€“ Also, if sorption/filtration site density (Smax) is very large, then linear Kd-type approach works ๏ฎ Every linear equilibrium assumption reduces number of equations by one (sorbed or filtered species equation is eliminated) ๏ฎ Special case of all reactions being at equilibrium and having a steady-state colloid concentration, Ccol : 8 0=+ 2 2 x C CKv t C CK t C K+ x C D x C v t C colcfcolcd B cf โˆ‚ โˆ‚ + โˆ‚ โˆ‚ + โˆ‚ โˆ‚ โˆ‚ โˆ‚ โˆ’ โˆ‚ โˆ‚ โˆ‚ โˆ‚ ฯ† ฯ ( ) 0=1+1 2 2 x C D x C vCK t C CKK cfcolccolcd B โˆ‚ โˆ‚ โˆ’ โˆ‚ โˆ‚ + โˆ‚ โˆ‚ ๏ฃท๏ฃท ๏ฃธ ๏ฃถ ๏ฃฌ๏ฃฌ ๏ฃญ ๏ฃซ ++ ฯ† ฯ colc colcd B C CK CKK R + ++ = 1 1 ฯ† ฯ Solute Transport Eq.: Rearranged: Effective Solute Retardation Factor: Note Kd = kas/ksa, Kc = kac/kca 6/8/2016 CFT Lightning