RF contact non conformities in LHC interconnects: Impedance aspects N. Mounet, B. Salvant With the help of: Gianluigi Arduini, Vincent Baglin, Serge Claudet,

Slides:



Advertisements
Similar presentations
SPS impedance work in progress SPSU meeting August 11 th 2011.
Advertisements

Impedance of SPS travelling wave cavities (200 MHz) A. Grudiev, E. Métral, B. Salvant, E. Shaposhnikova, B. Spataro Acknowledgments: Erk Jensen, Eric Montesinos,
Impedance of new ALICE beam pipe Benoit Salvant, Rainer Wanzenberg and Olga Zagorodnova Acknowledgments: Elias Metral, Nicolas Mounet, Mark Gallilee, Arturo.
Vacuum, Surfaces & Coatings Group Technology Department Cleanness of the 3-4 cold beam lines Outline:  History: Status of 2009 cleaning  Foreseen and.
1 Presented at ColUSM by D. Ramos on behalf of the Cold Collimator Feasibility Study Working Group Longitudinal.
Outcome of yesterday’s brainstorming on the potential of using CALIFES or CTF3 electron beam for impedance studies Elias Métral, Benoit Salvant, Carlo.
ALIGNMENT OF Q2 LOW BETA QUADRUPOLES D. Missiaen, On behalf of the EN-MEF-SU/MTI team 1.
Particle Studio simulations of the resistive wall impedance of copper cylindrical and rectangular beam pipes C. Zannini E. Metral, G. Rumolo, B. Salvant.
TDI longitudinal impedance simulation with CST PS A.Grudiev 20/03/2012.
Impedance aspects of Crab cavities R. Calaga, N. Mounet, B. Salvant, E. Shaposhnikova Many thanks to F. Galleazzi, E. Metral, A. Mc Pherson, C. Zannini.
Beam Vacuum Quality Control Outline  VSC consolidation  VSC support  Organization  Status Cédric Garion on behalf of TE-VSC Cédric Garion TE/VSC Beam.
Studies of impedance effects for a composite beam pipe for the experimental areas Request from M. Galilee, G. Schneider (TE/VSC)
LSWG day: Impedance and beam induced heating Nicolas Mounet *, Daria Atapovych, Nicolò Biancacci, Elias Métral, Tatiana Pieloni, Stefano Redaelli, Benoit.
Status of the PSB impedance model C. Zannini and G. Rumolo Thanks to: E. Benedetto, N. Biancacci, E. Métral, N. Mounet, T. Rijoff, B. Salvant.
IMPEDANCE OF Y-CHAMBER FOR SPS CRAB CAVITY By Phoevos Kardasopoulos Thanks to Benoit Salvant, Pei Zhang, Fred Galleazzi, Roberto Torres-Sanchez and Alick.
Updated status of the PSB impedance model C. Zannini and G. Rumolo Thanks to: E. Benedetto, N. Biancacci, E. Métral, B. Mikulec, N. Mounet, T. Rijoff,
Update of the SPS transverse impedance model C. Zannini, G. Rumolo, B. Salvant Acknowledgments: H. Bartosik, O.Berrig, F. Caspers, E. Chapochnikova, G.
Update on BGV impedance studies Alexej Grudiev, Berengere Luthi, Benoit Salvant for the impedance team Many thanks to Bernd Dehning, Massimiliano Ferro-Luzzi,
Update on BGV impedance August 1 st 2013 Alexej Grudiev, Berengere Luthi, Benoit Salvant for the impedance team Many thanks to Bernd Dehning, Massimiliano.
Update on wire scanner impedance studies
TDI impedance and power loss O. Aberle, F. Caspers, A. Grudiev, E. Metral, N. Mounet, B. Salvant.
Status from the collimator impedance MD in the LHC Collimation team:R. Assmann, R. Bruce, A. Rossi. Operation team:G.H. Hemelsoet, W. Venturini, V. Kain,
Chromaticity dependence of the vertical effective impedance in the PS Chromaticity dependence of the vertical effective impedance in the PS S. Persichelli.
Injection Energy Review D. Schulte. Introduction Will review the injection energy So could answer the following questions: Which injection energy can.
News and hot topics Impedance meeting 14/04/2014.
Heat load analysis for Inner Triplet and Stand Alone Modules H. Bartosik, J. Hulsmann, G. Iadarola and G. Rumolo LBOC meeting 28 October 2014 Based on.
Update on TCTP heating H. Day, B. Salvant Acknowledgments: L. Gentini and the EN-MME team.
Elias Métral, LHC Beam Commissioning Working Group meeting, 30/11/2010 /241 PRELIMINARY FINDINGS FROM INSTABILITY MEASUREMENTS DURING THE 75ns AND 50ns.
FCC-hh: First simulations of electron cloud build-up L. Mether, G. Iadarola, G. Rumolo FCC Design meeting.
Vacuum, Surfaces & Coatings Group Technology Department 22 nd January 2015 C. Garion2 Beam Line Interconnection: snapshot of present design principles.
1 Update on the impedance of the SPS kickers E. Métral, G. Rumolo, B. Salvant, C. Zannini SPS impedance meeting - Oct. 16 th 2009 Acknowledgments: F. Caspers,
Update on new triplet beam screen impedance B. Salvant, N. Wang, C. Zannini 7 th December 2015 Acknowledgments: N. Biancacci, R. de Maria, E. Métral, N.
Proposal to change bunch length during physics fills to assess beam induced heating after LS1 M. Barnes, P. Baudrenghien, A. Burov, S. Claudet, S. Jakobsen,
A first glance at the impedance of an SPS collimation system Nicolas Mounet, Benoit Salvant, Carlo Zannini Acknowledgments: collimation team (Daniele,
August 21st 2013 BE-ABP Bérengère Lüthi – Summer Student 2013
Longitudinal impedance of new RF fingers O. Berrig, C. Garion, B. Salvant.
200 MHz option for HL-LHC: e-cloud considerations (heat load aspects) G. Iadarola and G. Rumolo HLLHC WP2 meeting 03/05/2016 Many thanks to: K. Li, J.
Update on the TDI impedance simulations and RF heating for HL- LHC beams Alexej Grudiev on behalf of the impedance team TDI re-design meeting 30/10/2012.
Pros and Cons of the 200 MHz System G. Iadarola, K. Li, E. Metral, G. Rumolo Thanks to: L. Medina, J. Esteban Mueller, B. Salvant, E. Shaposhnikova, R.
General – mode matching for transverse impedance being compared with CST and infinitely long pipes (Nicolo) – Carlo found a way to disentangle direct space.
Feasibility of impedance measurements with beam N. Biancacci, N. Wang, E. Métral and B.Salvant COLUSM meeting 27/05/2016 Acknowledgements: A. Lafuente.
Geometric Impedance of LHC Collimators O. Frasciello, S. Tomassini, M. Zobov LNF-INFN Frascati, Italy With contributions and help of N.Mounet (CERN), A.Grudiev.
Heat load estimates for the Long Straight Sections of the HL-LHC
Finemet cavity impedance studies
Update on HL-LHC triplet fingers
Benoit Salvant, Kyrre Sjobak, Christine Vollinger, Na Wang
Little module (HeatLoadCalculator) available at:
N.Biancacci, E.Métral, B.Salvant
Follow-up of HL-LHC Annual meeting
Laser-engineered surface structures (LESS) What is the beam impedance?
LHC at 7 TeV/c: comparison phase 1 / IR3MBC
CST simulations of VMTSA
Dummy septum impedance measurements
E. Métral, N. Mounet and B. Salvant
Update of the impedance of new LHC experimental beam pipes
TCTP the CST side F. Caspers, H. Day, A. Grudiev, E. Metral, B. Salvant Acknowledgments: R. Assmann, A. Dallocchio, L. Gentini, C. Zannini Impedance Meeting.
Beam impedance of 63mm VM with unshielded Bellows
Impedance working group update 3rd Sept 2013
Laser-engineered surface structures (LESS) What is the beam impedance?
E. Metral, G. Rumolo, B. Salvant, C. Zannini (CERN – BE-ABP-LIS)
Status from the collimator impedance MD in the LHC
Discussion on the TDI impedance specifications
LHC SPS PS Impedance working group update 3rd July 2013 HL-LHC:
Beam impedance of 63mm VM with unshielded Bellows
impedance aspects for the beam screen
HBP impedance calculations
Status of the EM simulations and modeling of ferrite loaded kickers
FOLLOW-UP FOR THE TCDQ & TCDS & TDI concerning the RF fingers
Impedance working group update 07th August 2013
Two beam coupling impedance simulations
Presentation transcript:

RF contact non conformities in LHC interconnects: Impedance aspects N. Mounet, B. Salvant With the help of: Gianluigi Arduini, Vincent Baglin, Serge Claudet, Cedric Garion, Massimo Giovannozzi, Alexej Grudiev, Leszek Hajduk, Elias Métral, Mirko Pojer, Mike Struik, Laurent Tavian LBOC – 17 Sept. 2013

Agenda Context Observations of non-conformities – QQQI.2R5 – QQBI.29R5 – QBBI.B19R3 (V2) Analysis: – what do we think happened? – What do we need to conclude from impedance point of view? – Were there issues during the run? Recommendation from impedance point of view

Context 3 interconnects (so far) found with contact fingers sticking in the beam pipe were found: – QQQI.2R5 (4 contacts between Q1 and Q2a) found in March 2009 (EDMS: ) – QQBI.29R5 (5 contacts between quadrupole and dipole) found in April 2013 (EDMS: ) – QBBI.B19R3 (11 contacts between 2 dipoles) found in August 2013 (EDMS: ) So far this year, 2 PIMS were found with this type of issue out of an order of 150 to 200 PIMS examined by endoscopy (for a total of ~3400 PIMS). RF contact strip

Agenda Context Observations of non-conformities – QQQI.2R5 – QQBI.29R5 – QBBI.B19R3 (V2) Analysis: – what do we think happened? – What do we need to conclude from impedance point of view? – Were there issues during the run? Recommendation from impedance point of view

Observation of non-conformities Only view from inside the beam pipe thanks to endoscope inserted several meters or tens of meters away X-ray analysis and tomography is not possible as there is too much metallic material around the RF contacts.

QQQI.2R mm  Plug in module between Q1 and stripline  Already seen in March 2009

QQQI.2R5 (1/3)

QQQI.2R5 (2/3)

QQQI.2R5 (3/3)

QQBI.29R5  Interconnect between quad Q29R5 and dipole A30R5 (PIM for beam 1)

QQBI.29R5

QBBI.B19R3  Interconnect between dipoles B29R3 and C19R3 (PIM for beam 1)

Agenda Context Observations of non-conformities – QQQI.2R5 – QQBI.29R5 – QBBI.B19R3 (V2) Analysis: – what do we think happened? – What do we need to conclude from impedance point of view? – Were there issues during the run? Recommendation from impedance point of view

Analysis What most likely happened? – Cedric Garion: in view of the geometry, the non-conformity occurred during initial mounting and not afterwards (i.e. not during operation or cool down/warm up). What do we need to give a recommendation from impedance point of view? – Did we lose contact between beam screen and PIM due to the non- conformity? – Is there a hole? – Is a cavity behind the beam screen visible by the beam due to the lack of contact? – What is the perturbation due to the RF contact sticking in the beam pipe

Potential damage? Conform Non conform: option 1 Non conform: option 2 Non conform: option 3 Other options? Most likely option

Analysis Did we lose contact between beam screen and PIM due to the non- conformity? – Following discussion with Cedric Garion, the contact should not be lost at the location of the RF contact strips as the beam screen is pressed against the PIM. Is there a hole? – A hole of twice the thickness of the RF contact can be there, but its depth is limited to 2.3 mm due to the other RF contacts present behind the screen  simulated by CST, should only lead to imaginary impedance in the frequency range of LHC but the impact is so small that the simulations detect only noise. Is a cavity behind the beam screen visible by the beam due to the lack of contact? – No, it should be closed, as there are RF contacts and ultimately the weld. What is the perturbation due to the RF contact sticking in the beam pipe?

Impact of non-conform RF contacts on the geometric impedance Impact of geometric protrusion on imaginary impedance, evaluated thanks to Kurennoy’s formula (Phys. Rev. E, 55 (3) 1997) for a half-ellipsoid: (for QQQI.2R5 transverse impedance we assume beta functions of 10km – pessimistic) As a percentage of the total geometric impedance budget (i.e. not taking into account resistive-wall impedance) at injection, we get: If any, impact of possible hole is small as well: as a comparison, the pumping holes of the arc beam screens on a length of 1m cover an area ~100 times larger and have an imaginary impedance of only ~0.06 k  /m. 18 QQQI.2R5QQBI.29R5QBBI.B19R3 Im(Z l /n) 0.3   Im(Z t ) 1.2 k  /m  k  /m  k  /m QQQI.2R5QQBI.29R5QBBI.B19R3 Longitudinal % % Transverse0.09 %0.001 %0.02 % Nicolas Mounet → Impact on LHC geometric impedance of these single non-conformities seems negligible.  No real longitudinal impedance expected up to 3 GHz  no heating

Agenda Context Observations of non-conformities – QQQI.2R5 – QQBI.29R5 – QBBI.B19R3 (V2) Analysis: – what do we think happened? – What do we need to conclude from impedance point of view? – Were there issues during the run? Recommendation from impedance point of view

Were there issues during the run? Vacuum? – Vincent Baglin said that nothing special was seen around these locations, but the measurement lacks spatial resolution Heat load to cryostats – Laurent Tavian looked at the heat loads to the beam screen and saw nothing special at these locations (here example for 29R5) – However, measurement is not very sensitive (as integrated)  No obvious heating issue during the run (as expected), but not many observables are sensitive enough

Did the situation get worse during LHC operation since March 2009? From what we can see, the answer seems to be no, the situation did not get worse. Again, as expected since no additional beam induced RF heating is foreseen. Endoscopy in 26 March 2009 Endoscopy in 28 August 2013

Agenda Context Observations of non-conformities – QQQI.2R5 – QQBI.29R5 – QBBI.B19R3 (V2) Analysis: – what do we think happened? – What do we need to conclude from impedance point of view? – Were there issues during the run? Recommendation from impedance point of view

Generally speaking, this type of non-conformities increase the impedance and should be corrected. The impact on impedance (longitudinal, transverse) and on beam induced heating of such individual non-conformities is expected to be negligible provided (1)we assessed correctly the extension of the damage. (2)there are not so many of these non-conformities as the integrated contribution can be significant.

Thank you for your attention!

Interconnect between Q1 and Q2 in IR5 123