Flange Insulation and Grounding in the SPS Jose E. Varela 06 October 2015.

Slides:



Advertisements
Similar presentations
Impedance Transformation. Topics Quality Factor Series to parallel conversion Low-pass RC High-pass RL Bandpass Loaded Q Impedance Transformation Coupled.
Advertisements

Filter Design (1) Jack Ou ES590. Outline Butterworth LPF Design Example LPF to HPF Conversion LPF to BPF Conversion LPF to BRF Conversion.
Characterization of Circuit Components Using S-Parameters Chapter 1.
SIMPLIFIED MODELS OF ILD AND SID DETECTORS: SIMULATIONS AND SCALED TEST ULB: Christophe Collette, David Tschilumba, Lionel SLAC: Marco.
Update on SPS BPM impedance B. Salvant for the 2008 impedance team.
1 ECE 3336 Introduction to Circuits & Electronics Note Set #12 Frequency Response More About Filters Spring 2015, TUE&TH 5:30-7:00 pm Dr. Wanda Wosik.
TRF Noise Floor Related Question Prepared by Bill Wu.
Part B-5 OSCILLATORS: Condition for oscillations. RC-phase oscillator with transistor and FET, Hartley and colpitts oscillators, Wien bridge oscillator,
Phys 272 Alternating Current. A.C. Versus D.C (Natural) Frequency, Period, etc…
STRIPLINE KICKER STATUS. PRESENTATION OUTLINE 1.Design of a stripline kicker for beam injection in DAFNE storage rings. 2.HV tests and RF measurements.
Carbon for SPS, state or the art and scrubbing runs, P.Chiggiato, P.Costa Pinto, P.Cruikshank, J.Ferreira Somoza, H.Neupert, A.Sapountzis, M.Taborelli,
Modelling of TPM noise problems Greg, following discussions and measurements with David and Senerath.
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.
Lecture 16 In this lecture we will discuss comparisons between theoretical predictions of radiation and actual measurements. The experiments consider simple.
USCEL Third Run EMI Round Robin Roland Gubisch Intertek.
ECG Monitor Objective o Provide users an economical ECG monitoring device o Raise awareness to the importance of a healthy heart and living o Allow doctors.
T. Argyropoulos, LIU /04/2013 Progress in the SPS: RF studies and beam quality T. Argyropoulos, T. Bohl, J. E. Muller,, H. Timko, E. Shaposhnikova.
Propagation in Photonic Crystal Coupled Cavity Waveguides Possessing Discontinuities Ben Z. Steinberg Amir Boag Orli Hershkoviz Mark Perlson Tel Aviv University.
Agenda: General kickers analysis Wang-Tsutsui method for computing impedances Benchmarks Conclusions Bibliography Acknowledgments: E.Métral, M.Migliorati,
Status of the SPS impedance model C. Zannini, G. Rumolo, B. Salvant Acknowledgments: H. Bartosik, O.Berrig, G. Iadarola, E. Métral, N. Mounet, V.G. Vaccaro,
Update of the SPS transverse impedance model Benoit for the impedance team.
IMPEDANCE OF Y-CHAMBER FOR SPS CRAB CAVITY By Phoevos Kardasopoulos Thanks to Benoit Salvant, Pei Zhang, Fred Galleazzi, Roberto Torres-Sanchez and Alick.
Yi HUANG Department of Electrical Engineering & Electronics
Update of the SPS transverse impedance model C. Zannini, G. Rumolo, B. Salvant Acknowledgments: H. Bartosik, O.Berrig, F. Caspers, E. Chapochnikova, G.
Shielding of the SPS Vacuum Flanges - Design Studies – Update Jose E. Varela and Jaime Perez 21 May 2015.
Update on wire scanner impedance studies
Non - Inverting Amplifier
W. Hofle LIU-SPS Meeting SPS BA2 Damper LS1 Progress and plans reported by W. Hofle LIU-SPS Meeting G. Kotzian T. Levens D. Valuch.
BEPCII Transverse Feedback System Yue Junhui Beam Instrumentation Group IHEP , Beijing.
LIU-SPS ZS Electrostatic Septum Upgrade Review held on M.J. Barnes & T. Kramer.
Some ideas for/from the SPS LIU-SPS team. Scrubbing (only) for ecloud in SPS? aC coating remains baseline..... –but scrubbing has many potential advantages.
SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.
Longitudinal HOM power estimations for pulsed beams.rev W. Weingarten 31 May 20101SPL Cavity WG Meeting.
Longitudinal Impedance Characterization of the SPS MBA-QF Unshielded Pumping Ports Simulations, bead-pull and wire measurements Fritz Caspers, Jonas Ghini.
LIU-SPS upgrade, schedule, target parameters and observed limits 1 B. Goddard, E. Shaposhnikova for LIU-SPS coordination team SPS scrubbing review
SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela Acknowledgements: Jose A. Ferreira and Thomas Bohl.
Variable-Frequency Response Analysis Network performance as function of frequency. Transfer function Sinusoidal Frequency Analysis Bode plots to display.
End-of-year talk LIU-SPS BD WG meeting Our meetings in 2015 O During year - 9 meetings of LIU-SPS BD WG (as in 2013, but 10 in 2014 and 12 in.
Reminder on longitudinal modes of the SPS BPMs and ZS pumping ports Benoit Salvant for the impedance team.
Impedance Working Group Update ICE meeting June 12 th 2013.
End-of-year talk LIU-SPS BD WG meeting Our meetings in 2013 O During year - 9 meetings of LIU-SPS BD WG (less than usual 12 in the past :-)
RF measurements during floating MD in Week 40 3 rd of October 2012 LIU-SPS BD WG 25/10/2012 Participants: T. Argyropoulos, H. Bartosik, T. Bohl, J. Esteban.
Outcome of beam dynamics simulations - Scenarios, requirements and expected gains s LIU-SPS Coordination meeting 26/08/2015 A. Lasheen, E. Shaposhnikova,
LIU-SPS Beam Dynamics WG E. Shaposhnikova LIU-SPS coordination meeting
Design of a direct conversion 200 MHz non-IQ scheme using the Dimtel LLRF4 card Bob Anderson.
SPS Enamelled flanges Simulations & Measurements Fritz Caspers and Jose E. Varela.
Summary of discussion on isolating flanges E. Shaposhnikova With input from LIU-SPS BD WG (in particular H. Bartosik, F. Caspers and J. Varela), K. Cornelis,
New Contributions to the SPS Longitudinal Impedance Model
SPS Longitudinal Impedance Simulations & Measurements Update Benoit Salvant, Carlo Zannini, Thomas Bohl, Helga Timko, Fritz Caspers, Elena Shaposhnikova.
Follow up of Soft clamps production & testing Thomas Kaltenbacher & Christine Vollinger LIU-SPS, 26/05/2016 Thomas Kaltenbacher.
LIU and TE/VSC activities LIU-SPS aC coating & flange impedance reduction Paul Cruikshank LIU & TE/VSC activities, 23/6/2016 Paul Cruikshank.
LIU and TE/VSC activities Status September 2016 LIU-SPS aC coating & flange impedance reduction Paul Cruikshank on behalf of TE-VSC LIU & TE-VSC, 19/9/2016.
Longitudinal impedance of the SPS
Bellows Vibrations in the 3.9 GHz Cryomodule
Follow up on SPS transverse impedance
Status of Vacuum Flange Shielding/ Comparison of RF-shielding Designs
Crab Cavity Manufacturing Readiness Meeting
Benchmarking the SPS transverse impedance model: headtail growth rates
Update on PS Longitudinal Impedance Model
FCC-ee: coupling impedances and collective effects
Transition Wakes in the 3.9 GHz Cryomodule
Status of the EM simulation of ferrite loaded kickers
Hour 12 Driven Harmonic Oscillators
SPS-DQW HOM Measurements
TCLIA/TCTV transverse BB impedance versus gap size
Chapter 8.1 Chapter 8.2 PERIODIC STRUCTURES
Results on RF-Measurements on 3-Convolution HL-LHC fingers
Kirchhoff's Rules There are two KIRCHHOFF'S RULES. 1. Junction rule 2. Loop rule These are useful in circuit analysis.
Update on the SPS Impedance Model
TCLIA/TCTV transverse BB impedance versus gap size
Presentation transcript:

Flange Insulation and Grounding in the SPS Jose E. Varela 06 October 2015

Outline Overview of present situation for enameled flanges Implications for Impedance Conclusions

Overview of the present situation for enamelled flanges The main source of enamelled flanges in the SPS are the, approximately, 100 BPHs and 100 BPVs. Each has two enamelled flanges. Flange group #1Number Enamelled QD – QD 103 Enamelled BPV – QD 94 Non-enamelled QD – QD 69 PP – Long QD Bellows 76 PP - VVSA – Long QD Bellows17 Special Positions Group I 33 TOTAL 392 Flange group #2Number Enamelled QF – MBA82 Enamelled MBA – MBA14 Enamelled BPH – QF40 (104) Non-enamelled QF – QF27 Non-enamelled QF – QF No Bellows 21 Unshielded PP MBA - QF17 Special Positions Group II38 TOTAL239 (303) Flanges currently accounted for in the longitudinal impedance model. (Simplified classification - Only SSS accounted for)

Overview of the present situation for enamelled flanges Current longitudinal impedance model for the flanges. NOTE Below ≈50MHz the contribution of the enamel flanges is unknown.

Below ≈ 50 MHz, the impedance of enamelled flanges is not known. Enamelled flanges resonate somewhere between 1 and ≈50MHz This was reported several times in the past after tunnel and lab measurements. Overview of the present situation for enamelled flanges This ‘low frequency’ resonances were not considered to be important.

Measurement on the ENAMELLED flange LIU-SPS BD meeting Imaginary Part of the reflection coefficient

Measurement on the NON-ENAMELLED flange LIU-SPS BD meeting Imaginary Part of the reflection coefficient

Outline Overview of present situation for enameled flanges Implications for Impedance Conclusions

Implications for Impedance Right now, we would have higher impedance without enamel. Could be much worse without damping resistors.

Implications for Impedance Currently, we have: Low frequency effects: Unknown/Not quantified High frequency effects: On first order approximation, the enamel layer damps the resonances. Thus non- enamelled flanges have higher Q and higher impedance. QD flanges would have a much higher impedance if the enamel is removed (Q would go from 80 to 1000 for the 1.7GHz resonance). Depending on the action: If the enamel is removed somehow: The low frequency resonance would disappear. The flanges would have ‘much’ higher impedance (especially the QD ones). Shielded/Redesigned flanges would be almost unaffected. If some sort of low pass filter is implemented: The low frequency resonance would disappear. The high frequency impedance would be unaffected.

Outline Overview of present situation for enameled flanges Implications for Impedance Conclusions

There are around 400 enamelled flanges (mainly, 2 per BPM). The low frequency impedance of enamelled flanges is not known/ has not been quantified. We do know that there is a low frequency resonance (between 1 and 50MHz). Impedance wise, the enamel basically damps the flange resonances (significantly). It is thus, a potential source of EMC/EMI problems (as Fritz has pointed out many times). Depending on the way in which the enamel is ‘removed’, impedance could go up significantly. If some sort of low pass filter is implemented, the high frequency impedance would remain unaffected. Even if the enamel is completely removed, the shielded/redesigned flanges would be fine with it.