Hot Topic: Source(s) of Cavity Quench What Causes Surface Pits? Why Do Some Cause Quench? Lance Cooley Fermilab.

Slides:



Advertisements
Similar presentations
New Optical Inspection Results at JLab An in-depth update since Chicago meeting ILC08 (Highlights reported in US Regional Talk by Mark Champion) Rong-Li.
Advertisements

Stainless Steels Stainless steels are iron base alloys that contain a minimum of approximately 12% Cr, the amount needed to prevent the formation of rust.
Presented by Grigory Eremeev Grigory Eremeev. Presented by Grigory Eremeev Outline: - Cavities and Fields; - Results; - Tricks of the Trade: new shapes;
The Structure of Metals
Corrosion & Associated Degradation
Recent Surface Studies in KEK-STF
ILC PM Meeting S0 Webex Global Design Effort 1 S0/S1 Next Steps Lutz Lilje GDE.
Superconducting RF Materials University Collaboration STATUS Lance Cooley June 07, 2010.
Cooley – Main Linac ILCTA 1 Summary of the SRF Materials Workshop held October at Michigan State Univ. hosted by MSU, NSCL, and Fermilab
Chapter 5 - Imperfections in Solids
Cavity status; recent KEK activities : Hayano (1) STF CM-1 cavities are; MHI-014: 3-rd VT:36MV/m (finished) MHI-015: 3-rd VT: > 18.4MV/m.
Superconducting rf test facility STF 1 Optical Inspection update at KEK Ken Watanabe ( KEK ) ILWS08 in Chicago 17-Nov-08.
IMPERFECTIONS IN SOLIDS
1 UN1001: REACTOR CHEMISTRY AND CORROSION Section 11: Hydrogen Effects By D.H. Lister & W.G. Cook Department of Chemical Engineering University of New.
CAVITY TREATMENT (BCP, HEAT TREATMENT & HPR) Sergio Calatroni with many contributions from: Rama Calaga, Leonel Ferreira, Antonio Mongelluzzo LHC CCEM,
R.L. Geng, 5/27-31,2013 ECFA LC2013, DESY 1 Update on Raising Q0 at Ultra-High Gradient via Large-Grain Niobium Material Rongli Geng Jefferson Lab ECFA.
Advances in Large Grain Resonators Activities of DESY, W.C. Heraeus and RI material and fabrication aspects preparation and RF test results W. Singer,
Americas Cavity Specification C.M. Ginsburg (Fermilab) On behalf of the Fermilab cavity crew October 20, 2010.
Superconducting rf test facility LCWS 2010 in Beijing, 28 Mar 2010, Ken Watanabe Replica-method and local grinding repair K. Watanabe (KEK) LCWS 2010 in.
Update on S0 Work in the Americas Region Mark Champion 17 June 2008.
Study of heat and chemical treatments effects on the surface of ultra-precision machined discs for CLIC X-band Accelerating Structure Review (24 Nov. 2014)
A confocal Raman microprobe analysis of partial discharge activity in gaseous voids N A Freebody 1*, A SVaughan 1, G C Montanari 2 and L Wang 2 1 University.
© 2009 Al-Abdallat Properties of Eng. Material 1 (3) Interfacial defects Interfacial defects: Types: External surfaces, Grain boundaries, Twin boundaries.
Curtis Crawford, Georg H. Hoffstaetter Cornell University Laboratory for Elementary-Particle Physics Optimization of f 9-cell Vertical Electro Polishing.
Summary of Results and Development of Online Monitor for T-mapping/X-ray-mapping in KEK-STF Y. Yamamoto, H. Hayano, E. Kako, S. Noguchi, M. Satoh, T. Shishido,
How important is the surface finish/roughness in determining the performance of Nb cavities? Introduction Peter Kneisel Jlab.
High Temperature Heat Treatment to Raise the Quality Factor of Large Grain Niobium Cavities Pashupati Dhakal Gianluigi Ciovati Ganapati Rao Myneni July.
Scanning Tunneling Microscopy Studies of Single-Crystal Niobium Oxidation Natalie A. Kautz, Yichen Yu, Kevin D. Gibson.
Centrifugal Barrel Polishing at Fermilab (Tuesday, December 6th at 10:20) Tesla Technology Collaboration IHEP, Beijing December 5 th -8 th, 2011.
Genesis of topography by buffered chemical polishing of niobium Liang Zhao, Taina Matos, Tina Wang, Josh Spradlin, Charles E. Reece, Michael J. Kelley.
Update on S0 Work in the Americas Region Camille Ginsburg (FNAL) 2 June 2009 Slides/Info from: Zack Conway (Cornell) Rongli Geng (JLab) Genfa Wu, Dmitri.
Andrew BurrillFall 2011 Project X Collaboration Meeting 650 MHz Developments at JLAB Andrew Burrill for the JLab Team.
Corrosion process and control (TKK-2289)
Superconducting Magnets and Materials: Superconducting Materials for RF Applications Lance Cooley – Head, SRF Materials Group Fermilab General Accelerator.
Raw Materials Specifications and Material Batch History (Niobium sheets used to make 9-cell cavities) Lance Cooley Head, Superconducting Materials Department,
1 Guided Cavity Repair with Laser, E ‐ Beam and Grinding Genfa Wu Recent cavity processing statistics indicate that the development of RF superconductivity.
Possible Relationship Between Defect Pre-Heating and Defect Size H. Padamsee Cornell S0 Meeting, Jan 26, 2009.
Plasma cleaning Laser re-melting technique at FANL M. Ge, G. Wu, J. Ruan, J. Ozelis, T. Nicol, D. Sergatskov, D. Hicks, L. Cooley Fermi National Accelerator.
Rongli Geng ILC Cavity Group Meeting October 25, 2011
HYDROGEN EMBRITTLEMENT : CAUSES, EFFECTS & PREVENTION ABHISHEK KUMAR BT/ME/1601/002.
Electropolishing of Dressed ILC 9-cell Cavity
Condition of electron beam welding toward a high gradient application
DR S. & S. S. GHANDHY GOVERNMENT ENGINEERING COLLEGE , SURAT.
Energy (ILC) and Intensity (Project X) SRF Cavity Needs
Vertical Electropolishing at Marui & KEK
Ashwini Chandra M.D. Sumption, E.W. Collings G.S. Frankel
Lance Cooley Monday morning meeting 27 September 2010
Corrosion process and control (TKK-2289)
Surface Analysis of the Quench Area Sample of Cavity Z111
ENT 487 ENVIRONMENTALLY ASSISTED CRACKING IN METALS
Fabrication of Nb and Cu SPL cavities and required tools CERN status
High Q via N infusion R&D at Jefferson Lab
High Q R&D at Fermilab Anna Grassellino TTC Topical Meeting on CW SCRF
Some History of Electropolishing of Niobium 1970 – 1990
VERTICAL TEST RESULTS OF SPOKE RESONATOR AT IPNO
Manufacturing Processes
A COMMON R&D ON THE HIGH GRADIENT Nb CAVITIES
R&D Activity for Field Emission and Vertical EP
TTC High Q0 Working Group Summary of developments since last TTC meeting C. Reece.
Manufacturing Processes
Mechanisms in the Cleaning of Aluminium Melts with Flux Preparations
Dislocations Dislocations Dislocations
Physical and Chemical Changes
Corrosion & Associated Degradation
SRF Surface Studies and the High Field Q-slope Mystery
Principle of the process Design For Manufacturing (DFM)
TTC Meeting, 28 February - 2 March, 2011, Milan
CHAPTER 4: IMPERFECTIONS IN SOLIDS
JLab Work on Low Temperature Near-Surface Diffusion aka “Infusion”
Prepared By: Mr. Prashant S. Kshirsagar (Sr.Manager-QA dept.)
Presentation transcript:

Hot Topic: Source(s) of Cavity Quench What Causes Surface Pits? Why Do Some Cause Quench? Lance Cooley Fermilab

Crime Scene Investigations – How did pits form? Shape and topography of defects:  Hemispheres – bubbles of gas trapped during solidification, etching at electrolyte bubble edges  Facets – Grain-boundary stress, directional etching  Bumps – Spatter (due to what?)  Other – Incomplete weld? Foreign matter? Location of defects relative to welds:  In re-solidified zone – bubbles  In recrystallized zone – stress, directional attack  At edge of HAZ – dislocation- assisted etching, impurity pockets, machining debris  Elsewhere – “flash” reaction of acid with water droplet Composition of defects  Carbon, oxygen, hydrogen contaminants  (Need more data) Lance Cooley, Fermilab – SRF'11 Hot Topic, 25 July 20112

Do we create bubbles, or uncover them? Hemispheres in re-solidified zone - Bubbles formed during welding and became trapped  That is, processing uncovers them  Do bubbles flow along e-beam direction? If so, weld from the inside of the cavity  Local grinding or re-melting may be favored over bulk removal, such as CBP or EP, due to risk of uncovering other bubbles  Is tomography accurate enough to screen welds? Hemispheres in other zones – Corrosion pitting  That is, processing creates them  Sulfuric acid flash-reacting with water droplets  Re-processing should repair them Lance Cooley, Fermilab – SRF'11 Hot Topic, 25 July 20113

Can bubbles come from weld-prep etch? 2% H is typical level after 20 µm BCP, based on bulk spectroscopy data With 40 µm grains, then mol H can collect at grain-boundary triple points during heat-up Assuming H is ideal gas, a bubble then can contain 2.5 µJ energy at 3000 K Given surface tension of molten niobium ~2 J/m 2 (NIMS data), the equilibrium bubble radius is approximately 300 µm  This is what is routinely seen! Implication: change the pre-weld etch to a “flash” etch, keep it cold, and perhaps consider a de- gassing bake Lance Cooley, Fermilab – SRF'11 Hot Topic, 25 July 20114

Facets and directional attack Welding concentrates dislocations (DLs) & impurities at the HAZ edge, sensitizing metal to pitting  That is, processing creates the defects, and re- processing will continue to create more defects  Grain-boundary junctions and grain orientations with emerging DLs may be troublesome Cold work promotes dislocation-assisted pitting  Therefore, is it prudent to anneal half cells before welding?  800 °C bake produces recovery, but also concentrates DLs into walls via polygonalization Temperature increase during EP promotes fluorine mixing, which breaks down viscous salt film  Supply of fluorine to surface then produces attack where DLs are concentrated Lance Cooley, Fermilab – SRF'11 Hot Topic, 25 July 20115

Further deleterious properties of dislocations Dislocations attract hydrogen and bind it  Hydride precipitates are present at room temperature and may remain stable despite 120 C baking Hydrogen bound to DLs expands lattice and promotes further formation of DLs, and hence further uptake of hydrogen  This is a common mechanism of hydrogen embrittlement RF currents induced to flow across precipitates produce dissipation, resulting in Q drop So, if DLs are present at the bottom of etch pits, they provide an inherent loss source  That is, topographical features (such as the pit rim) may be less important for Q limit. Pits without dislocations could be benign. Lance Cooley, Fermilab – SRF'11 Hot Topic, 25 July 20116

A pit uncovered by EP August 6, 2010ASC 2010 – Washington D.C. 5MZ-017 As Received After 1 st EP After 2 nd EP Electropolishing of an iris weld reveals (creates?) a nearly hemispherical pit. And, as with other pits, it is at the boundary of the weld bead. Images courtesy of Dmitri Sergatskov, FNAL

Breakdown of viscous salt film by dunking coupon during EP resulted in many large pits along HAZ edge August 6, 2010ASC 2010 – Washington D.C. 5MZ-018

Recovery anneal reduces tendency for attack somewhat, but also seems to concentrate DLs Lance Cooley et al., Fermilab – 2011 CEC/ICMC Presentation M1OrC-069 CW + weld °C 1 cm x 1 cm Weld HAZ CW + weld °C 1 cm x 1 cm Weld HAZ See THPO075 New tool: Laser Confocal Scanning Microscopy

Connection between Q-slope (onset above 100 mT) and small near-surface hydride precipitates! Lance Cooley, Fermilab – PAC11, 31 March A. Romanenko, Fermilab, See THPO008 These are hydrides: Vinnikov and Golubok, Phys. Stat. Sol. 69:631 (1982) and others

Evidence for NbH and Nb 3 H 4 at dislocations B Albee, D Ford et al, THPO060 Lance Cooley, Fermilab – SRF'11 Hot Topic, 25 July Black: Raman spectroscopy data – B. Albee et al, IIT Vertical lines – density-functional calculations, D. Ford, FNAL/NWU

Laser melting also produces a HAZ like a weld SEM with orientation imaging shows pile-up of DLs at grain boundaries. Subsequent etching attacks the metal preferentially at these regions  Dzyuba et al, THPO051 Lance Cooley, Fermilab – SRF'11 Hot Topic, 25 July

Summary – Hot topic It is plausible that hydrogen bubbles form in the molten weld due to pre-weld etching.  Use “flash” etching, keep cold, minimize H uptake Plausible mechanisms exist for BOTH uncovering pits and creating them during processing.  Maintain efforts on local repairs and processing R&D Dislocations harbor hydrogen and assist chemical attack.  Use baking to recovery or recrystallize  Hydrides produce Q loss – smoking gun: DLs near pit Avoid breakdown of EP salt film (cold EP). If breakdown occurs, it can be tolerated if the metal is not sensitized to attack. Lance Cooley, Fermilab – SRF'11 Hot Topic, 25 July