ucla - s.sharafat: iter tbm dec. ’04 dcll iter-tbm: design for accident relevant loading jaafar a....

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UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem, University of California Los Angeles ITER-TBM Meeting UCLA March 2-5, 2005

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Page 1: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

DCLL ITER-TBM:Design for Accident Relevant

Loading

Jaafar A. El-Awady, P. Rainsberry,S. Sharafat, and N. Ghoniem,

University of California Los Angeles

ITER-TBM MeetingUCLA

March 2-5, 2005

Page 2: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Outline

Model of Dual Coolant Lead Lithium (DCLL) Test Blanket Module.

“Back of the Envelope” FEM to determine design features, most relevant to accident loading.

Detailed FEM analysis Results.

Design Modifications based on FEM analysis.

Page 3: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Dual Coolant PbLi Concept

1940ModuleHeight

38Top Plate

38Bottom Plate

First Wall

Mo Dagher,Mar.1st

Page 4: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Accident Simulation

An accident scenario is simulated for a leakage of Helium into DCLL-TBM

Structural analysis was performed with the following conditions:

Leakage of 8 MPa Helium into DCLL-TBM, thus increasing the pressure in the breeder channels to 8 MPa

Extreme temperature conditions (T = 650oC) is applied as a uniform temperature on the entire DCLL-TBM

Page 5: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Model for Back-of-the Envelope” FEM

8 MPa

Boundary ConditionsBack wall constrainedfrom moving in the horizontal Plane but free to expand in the vertical direction

Extreme Temperatures appliedT = 650oC

FEM

8 MPa

Back Wall

First Wall

Horizontal plane

Vertical direction

Page 6: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

“Back-of-the Envelope” Structure Analysis

Page 7: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

“Back-of-the Envelope” Structure Analysis

8 MPa

Alternating Pattern of high stresses

“shadowing” internal FW tube Structure:

Maximum Stress= 524.19 MPa

Page 8: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Back-of-the-Envelope FEM Summary

FE Models must include Detailed Design of the FW and Supporting Ribs to identify critical design features.

“Back of the Envelope” FEM shows the weakest “link” to be the edges between the FW and the internal support structure.

Internal support structure – FW bonds will take the DCLL module beyond allowable stresses of 300 MPa at elevated temperatures.

Page 9: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Detailed FEM Analysis

Page 10: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Detailed FE-Model• A 3-D solid model of the TBM was created, including all of the FW channels.

• Over 200K elements.• Symmetry boundary conditions where applied to simulate the entire TBM

Meshed model showing internal support structures and FW-Channels

Page 11: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Structure Analysis Results

Displacements:

Maximum Displacements occur at the tips and is equal to

8.435 mm

Back View

IsoFront View

Page 12: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

True Model Structure Analysis ResultsStress Distribution:

= 530 MPa

Critical section 1:(Rib-first wall)

View A

View A

Page 13: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

True Model Structure Analysis ResultsCritical section 2: (top plate – first wall connection)

View B

= 616 MPa

Looking from the inside up at the top PLATE

Top Plate

FW (from the inside)

Rib (not all the way totop Plate

Page 14: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Channeled FW to Equivalent “Solid” FW

Stresses:

Equivalent Model with effective thickness for same stress

True Model

While the transformed model gave an average stress distribution equivalent to the true model, it wasn’tcapable of capturing the critical sections were the

stresses have doubled (these sections will be described in the following slides).

Page 15: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Reinforced Rib-FW Structure

Adding more material between top Channel of FW and Top Plate (4 mm)

Page 16: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Reinforced Rib-FW Contact Model: Structure Analysis

Max: ~415 MPa

Max: ~8 mm

Front view

Back view

Page 17: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Reinforced Rib-FW StructureAdding material (4x4 mm)

Reduced Maximum Stresses from

530 MPa to 450 MPa

= 450 MPa

First Wall

Added material

Page 18: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Reinforced Top Plate Side Wall Contact

= 415 MPa

Adding material (4x15 mm) Reduced Maximum

Stresses from 616 MPa to 415 MPa

Page 19: UCLA - S.Sharafat: ITER TBM Dec. ’04 DCLL ITER-TBM: Design for Accident Relevant Loading Jaafar A. El-Awady, P. Rainsberry, S. Sharafat, and N. Ghoniem,

UCLA - S.Sharafat: ITER TBM Dec. ’04

Summary

The entire DCLL TBM including FW channel detail was modelled for an over pressurization analysis (8 MPa).

Stress distribution on support structure/FW contact areas shows “shadowing” of FW channel detail on stress states.

Without reinforced support structure FW and Top/Bottom Plate contact areas, stresses are high.

Modifying internal Rib-FW/Top/Bottom-Plate contact areas can reduce maximum stresses significantly.

Details of the most optimized reinforcement design are yet to be determined.