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(1) Die Kooperation von Forschungszentrum Karlsruhe GmbH ... New geometrical model of EFIT core in SIMMER-III. Coolant outlet. Coolant inlet. Coolant flow pass ... – PowerPoint PPT presentation

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1
IP EUROTRANS DM1
Transient Analysis for the EFIT 3-Zone Core
P. Liu, X.-N. Chen, A. Rineiski, S. Wang, M.
Flad, W. Maschek Forschungszentrum Karlsruhe,
IKET Postfach 3640, D-76021 Karlsruhe
IP EUROTRANS DM1 WP1.5 Mtg. Bologna, 28-30 May
2008
2
Contents
  • Design base and Some former work
  • (ULOF, Beam trip, UTOP, UBA already
    presented in last meeting)
  • SIMMER-III new model
  • (with a new implemented pump model)
  • ULOF (under new pressure drop conditions)
  • Beam Trip (short term beam trip1second)
  • Unprotected Blockage (first fuel ring totally
    blocked)
  • Summaries

3
ENEA 384MWth 3Zone Core Design
4
Former work-SIMMER-III simulation of the steady
state
SIMMER-III
5
Former work-SIMMER-III simulation of the steady
state
SIMMER-III Calculated Peak Fuel
Temperature 1352.1 ? Peak Clad Temperature
521.1 ?
Limit temperatures at nominal conditions Fuel
1380 ?, Clad 550 ? (From ENEA Files)
6
New geometrical model of EFIT core in SIMMER-III
Coolant inlet
7
ULOF analysis
  • Assumptions and conditions
  • Core - SG midplane distance 3.7 m
  • The transient starts at 60 s from a well
    established steady-state
  • Total pressure drop in the primary system
  • 1.1 bar
  • 1.37 bar (two cases)
  • 1.87 bar
  • Pump head becomes zero in 10 s halving time 2
    s (Main)
  • Pump head becomes zero in 5s, halving time 2 s
  • (for the 2nd case of 1.37bar)

8
ULOF analysis -1.1 bar pressure drop
Pump head becomes zero in 10 s,
halving time 2 s
9
ULOF analysis -1.37 bar pressure drop (1st case)
Pump head becomes zero in 10 s,
halving time 2 s
10
ULOF analysis -1.37 bar pressure drop (1st case)
Simple view of the Coolant Movement in the system
during the pump coast down process.
11
ULOF analysis -1.37 bar pressure drop (2nd case)
Pump head becomes zero in 5 s, halving time 2
s Pump coast down data needed!!
12
ULOF analysis -1.87 bar pressure drop
Pump head becomes zero in 10 s,
halving time 2 s
13
ULOF-Comparison
14
Beam trip analysis
Assumption External beam amplitude being zero
for 1 second.
  • Fuel temp. at core mid-plane
  • Coolant and clad temp. at core outlet
  • Maximum fuel temp. decrease about 554 K
  • Maximum clad temperature decrease
  • about 14 K
  • Maximum coolant temperature decrease about 12 K.

15
Unprotected blockage
  • Assumptions/Conditions/Parameters
  • Innermost ring totally blocked
  • Transient starts at 30 s from a well established
    steady-state
  • He fission gas pressure (1MPa BOC initial at
    gas plenum)
  • Radial heat exchange between SA rings is taken
    into account
  • Clad failure and gas release at 1280K
  • Clad weakening and start of fuel movement at 1513
    K
  • Hexcan crack at 1280K
  • Hexcan weakening at 1513K
  • Fuel particle size volumetrically equals to one
    pellet r 4.555mm
  • Steel particle size r 2.0mm
  • No-removable upper pin structure
  • No damage propagation to Target facility

16
Unprotected blockage-Continued
  • Power increased to a maximum of 655 MW
  • Fuel pin damage propagation happens, damage
    spreads to the third fuel ring.

17
Summaries
  • ULOF Analysis
  • New SIMMER modeling on the ULOF has been
    performed with a pump and heat exchange region
    and in turn, the three free surface well modeled
    with the implemented pump model in SIMMER-III
  • Under the 1.37 bar total pressure drop and the
    assumed pump coast down conditions, the current
    core can survive the ULOF transient
  • Pump coast down data should be well established
  • Beam Trip Analysis
  • With a 1 seconds beam-off, the maximum fuel
    temperature decreases about 554 K, the maximum
    clad temperature transiently decreases 14 K, the
    maximum coolant temperature decreases 12 K
  • UBA Analysis
  • Fuel damage could happen and spread to the third
    fuel ring if the first fuel ring is completely
    blocked
  • The power can arrive as high as 655 MW
  • The power finally decreases due to the inherent
    fuel sweep-out mechanism.
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