Presented by Neil Morley University of California Los Angeles USEU DCLL Workshop November 1415 2014 Slides from my colleagues S Smolentsev and M Abdou gratefully acknowledged Next 10 Years ID: 760129
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Slide1
Multiple effects for HT DCLL
Presented by Neil Morley
University of California, Los Angeles
US-EU DCLL Workshop
November 14-15, 2014
Slides from my colleagues S.
Smolentsev
and M.
Abdou
gratefully acknowledged
Slide2Next 10 Years
We are now in mostly “Separate Effects” stage. We need to move to “multiple effects/multiple interactions” to discover new phenomena and enable future integrated tests in ITER TBM and FNSF
Now
TBMs in ITER & FNSF
in FNSF
Property Measurement
Phenomena
Exploration
Model Validation
Non-Fusion Facilities:
2
Theory/Modeling
Basic
Separate
Effects
Multiple Effect/
Interactions
Partially
Integrated
Integrated
Design Codes/Data
Component
Multiple Effects / Multiple Interactions
– bringing together different combinations of multiple physical loads, multiple materials and complex configurations that can drive new interacting and synergistic phenomena
Testing in Fusion Facilities
Slide3Consider a representative FW/blanket system:“Dual Coolant Lead Lithium” - DCLL
3
FW Armor
RAFS Structure
SiC Flow Channel
Inserts
Shield
He Flow
ARIES-ST DCLL
blanket
This is considered as a leading FW/Blanket system in the US
EU and China have similar version
Features and R&D issues are typical
of a family of
PbLi
and/or helium cooled FW/blankets
M
olten
PbLi
and helium coolants / breeders and circulation systems
Thermomechanical
response of helium cooled RAFS structures
Tritium transport and control
Corrosion and activation
Reliability over long operation and transient events
Slide4Features of the High Temperature DCLL
Allow high temperature PbLi flow inside FCI while keeping the RAFM steel operating in acceptable range for both structural and PbLi compatibilityKeep MHD pressure drop under control in a practical way that results in acceptable inboard dP and overall flow distribution
High temperature condition can be intentional for better power conversion or as a safety margin for temperature excursion protection
4
FCI
PbLi
He
Slide55
What do we think we need to know about DCLL MHD
thermofluid
multiple
e
ffects / multiple
i
nteractions
Slide6Combined MHD/heat/mass transfer behavior in a DCLL unit cell
Given a inflow conditions, non-uniform B-field and heating in typical DCLL unit cells, what will be the:Material interface temperatures, temperature gradients, thermal stressesMass loss rates and corrosion product concentrationsTritium transport rates and tritium concentrationsFCI performance and MHD Pressure dropWhat science needs to be studiedWhat combination of phenomena controls flow regime / stability of the channel. What is the sensitivity?How does the flow regime impact the heat and scalar transportE.g. Hot spots, corrosion product source terms, tritium leakage to helium, How does the FCI material properties and component integrity evolve over time due to interfacial effects
6
FCI
PbLi
He
Slide7Spatial Gradients in Nuclear Heating and Temperature in LM Blanket Lead to New Phenomena that fundamentally alter our understanding of the behavior of the blanket in the fusion nuclear environment
7
B
g
V
UPWARD FLOW
DOWNWARD FLOW
Vorticity Field
shows unstable velocity affecting all transport
phenomena
Base flow
strongly altered possibly leading to stagnant zones and “flow reversal”
Buoyant MHD interactions result in “Mixed Convection” flow regime
with substantial impact on flow dynamics, heat transfer, corrosion/tritium transport
Slide8The mixed-convection flow requires new rules for predicting transition.
Bottom: Flow map showing stable laminar (
s) and two turbulent regimes (wt and st) in the Ha – Re plane for Gr = 5x107.Top: Predictions of the critical Ha number with the linear theory.
Linear stability analysis
DNS
UCLA (
Smolentsev
) built
flow maps (Ha-Re-Gr) and
determined critical
Ha number to predict transitions and specify turbulence mode. These results suggest that in DCLL blanket (DEMO, Gr~1012) poloidal flows are turbulent.These predictions are so far limited to computations and analytical studies. Experiments are needed. We are planning such experiments. Pre-experimental analysis has been completed showing that anticipated flow regimes can be reproduced in the MTOR Lab.
Slide9Flow distribution in a complex, multi-material configuration of parallel channels
What design, flow conditions, and FCI behavior leads to highly unbalanced flow and channel overheating?Complex conducting structures, manifold designs and partial FCI insulation Magnetic fields not aligned with walls and will vary front-to-back, side-to-side and over time in large modulesHeating varies strongly back to front and vary over timeFCIs motion and property changes over timeUnsteady flows that may cause pressure oscillations
9
DCLL blankets modules have 4-8 multiple channels fed from common supply and return pipes
FW Armor
RAFS Structure
SiC Flow Channel
Inserts
Shield
He Flow
Slide10The current paths in complex flow elements are difficult to understand and predict, and will strongly impact flow distribution
10
In MHD one must always always be prepared to consider the complete electromagnetic field. The current and magnetic fluxes must have complete paths which may extend outside the region of fluid-mechanical interest into locations whose exact position may be crucial -- J A
Shercliff
UCLA current flow simulation in a 3 channel manifold, cut along symmetry plane down middle channel
Slide11PbLi ingress in SiC FCI can dramatically change conductivity, increase drag in that channel and lead to severe flow redardation
15
vol
% dense, 85% porosity filled with aerogel
Slide1212
What do we think we need to know about DCLL
t
hermofluid
multiple effects / multiple interactions
Slide13Next 10 Years
So how do we explore, discover, understand and accurately model multiple effect multiple interactions phenomena?
Now
TBMs in ITER & FNSF
in FNSF
Property Measurement
Phenomena
Exploration
Model Validation
Non-Fusion Facilities:
13
Theory/Modeling
Basic
Separate
Effects
Multiple Effect/
Interactions
Partially
Integrated
Integrated
Design Codes/Data
Component
Testing in Fusion Facilities
Use real materials, prototypic temperatures
Simulate surface and bulk heating and gradients
Provide large volume and use multiple channels
Have
more prototypic
Ha,
Gr, N, Re, etc.
A
handful of upgraded/new experimental facilities will be needed that:
Slide14We envision two thermofluid MHD facilities beyond near term upgrades of existing facilities
Multiple Effect/Multiple Interactions Blanket Facility Role: Address near full size DCLL unit cell thermofluid flow and transport issues and reduced scale multi-channel flow controlPartially Integrated Blanket FacilityRole: bring together all simulated conditions affecting thermofluid/thermomechanical blanket/FW performance to the maximal practical degree prior to FNSF
14
These are both non-nuclear facilities that can be flexibly operated and instrumented to investigate both prompt and long time scale DCLL blanket phenomena in a controlled and well characterized fashion
Slide15Blanket MHD thermofluid test facilities
Multiple Effect/Multiple Interactions Blanket Facility. Role: Address near full size DCLL unit cell thermofluid flow and transport issues and reduced scale multi-channel flow controlstrong magnetic field, ~5T Magnetic volume capable to accommodate full single channel size, ~0.3 x 1.5 m)controlled orientation with respect to gravity and channel wallssimulated volumetric heating and gradients PbLi and He flow loops at prototypic temperatures (~1/2 TBM scale)
15
$20M class facility, can be a gradual extension of MTOR/
MaPLE
facilities at UCLA
Slide16Possible upgrades for MaPLE and BOB magnet
Flexible B orientationHigher flowrate and temperature PbLiSimulated volumetricheatingOnline PbLi purificationInstrumentation
System to switch from Horizontal to Vertical oriented “BOB” magnet gap
Slide17Possible upgrades for MaPLE and BOB magnet
Flexible B orientationHigher flowrate and temperature PbLiSimulated volumetricheatingOnline PbLi purificationInstrumentationSecondary He coolantHigher magnetic fieldLarger magnetic volume
System to switch from Horizontal to Vertical oriented “BOB” magnet gap
Evolve into the Multiple Effect Multiple Interaction facility just described
Slide18Blanket MHD thermofluid test facilities
Partially Integrated Blanket Facility. Role: bring together all simulated conditions affecting thermofluid/thermomechanical blanket/FW performance to the maximal practical degree prior to FNSFSimulated toroidal and poloidal magnetic fieldUp to full size FW/blanket test modules in multiple poloidal orientations with respect to gravitySimulated surface and volumetric heating and gradients PbLi and He flow loop of ~full DEMO module sizePrototypic temperatures, pressures, materials
18
$50-80M class National Laboratory facility to really prepare for FNSF – requires significant design and construction effort
Slide19What are the principal challenges in simulating the fusion nuclear environment?
Nuclear heating in a large volume with strong gradients, not possible to reproduce in simulation facility. Use various techniquesEmbedded heaters in LM, on walls or in flow channel inserts. Must be careful about changing the flow, FCI behavior, etc. Integration into multiple experiments requiredInlet temperature control (e.g. flow in hot, let cool)Complex magnetic field with toroidal field / poloidal field fidelity or transient fields during disruptionsRequires complex magnet systems, very important for LM blanketsOr utilization of modules in long pulse confinement devicesComplex mockup configuration with prototypic size and scale Not possible in fission reactors
19
Can not bring together all conditions in one test or adequately simulate nuclear heating
Slide20Study on Blanket/FW Multiple Effect/Multiple Interaction and Partially Integrated Test Strategy and Facilities
20
Why the Study is Needed
The subject of multiple effect/multiple interactions is very complex and requires experienced blanket R&D experts
But the cost of the facility for full simulation can be very expensive
Therefore, tradeoffs between the capabilities incorporated in the facility and COST are needed. Developing cost estimates require mechanical design for a given set of specified parameters
Requires Blanket R&D experts as well as mechanical engineers and magnet designers and cost professionals. There are several US institutions interested in developing proposals to construct blanket facilities
The study could be “international” and a good mechanism for collaboration