KCS Operational Issues Chris Adolphsen, Chris Nantista and Faya Wang GDE PAC Review at KEK 12/12/12.

Slides:



Advertisements
Similar presentations
M. Ross Project Advisory Committee Review 13 December, 2012 KEK Main Linac Layout – Two variants for two different types of sites GDE PAC Review.
Advertisements

Breakdown Rate Dependence on Gradient and Pulse Heating in Single Cell Cavities and TD18 Faya Wang, Chris Nantista and Chris Adolphsen May 1, 2010.
11/27/2007ILC Power and Cooling VM Workshop Mike Neubauer 1 RF Power and Cooling Requirements Overview from “Main Linac Power and Cooling Information”
5th Collaboration Meeting on X-band Accelerator Structure Design and Test Program. May 2011 Review of waveguide components development for CLIC I. Syratchev,
Homework of HLRF 1 Shigeki Fukuda KEK 2012/4/23 HLRF Homework1 in KILC12 (Fukuda) 1.
KCS Ongoing R&D Christopher Nantista SLAC LCWS11 Granada, Spain September 29, …… …… …… … ….
Baseline Configuration - Highlights Barry Barish ILCSC 9-Feb-06.
3-March-06ILCSC Technical Highights1 ILC Technical Highlights Superconducting RF Main Linac.
Beam loading compensation 300Hz positron generation (Hardware Upgrade ??? Due to present Budget problem) LCWS2013 at Tokyo Uni., Nov KEK, Junji.
Demonstration of the Beam loading compensation (Preparation status for ILC beam loading compensation experiments at ATF injector in this September) (PoP.
Christopher Nantista ML-SCRF Technology Meeting July 28, 2010 REPORT.
Different mechanisms and scenarios for the local RF
RF COMPONENTS USING OVER-MODED RECTANGULAR WAVEGUIDES FOR THE NEXT LINEAR COLLIDER MULTI- MODED DELAY LINE RF DISTRIBUTION SYSTEM S. G. Tantawi, N. M.
Christopher Nantista Chris Adolphsen SLAC TILC09 Tsukuba, Japan April 20, 2009.
Christopher Nantista ILC 2 nd Baseline Assessment Workshop (BAW-2) SLAC January 18, …… …… …… … ….
Christopher Nantista 2011 Linear Collider Workshop of the Americas (ALCPG11) University of Oregon, Eugene March 20, …… …… …… … ….
RF Distribution Alternatives R.A.Yogi & FREIA group Uppsala University.
Gek 16/6/041 ITRP Comments on Question 19 GEK 9/06/04 19) For the X-band (warm) technology, detail the status of the tests of the full rf delivery system.
Test Facilities and Component Developments Sami Tantawi SLAC May 15, 2008.
Chris Adolphsen 10/03/09 MLI and HLRF Summary. Vladimir Kashikhin.
1 Results from the 'S1-Global' cryomodule tests at KEK (8-cav. and DRFS operation) Shin MICHIZONO (KEK) LOLB-2 (June, 2011) Outline I. 8-cavity installation.
Christopher Nantista ARD R&D Status Meeting SLAC February 3, …… …… …… … ….
Proposed TDR baseline LLRF design J. Carwardine, 22 May 2012.
Clustered Surface RF Production Scheme Chris Adolphsen Chris Nantista SLAC.
Klystron Cluster RF Distribution Scheme Chris Adolphsen Chris Nantista SLAC.
Linac R&D Update May 15, L-Band Source Consists of a LLRF system (VME/Epics based), a SNS High Voltage Converter Modulator (on loan), a Thales 2104C.
Vladimir Kashikhin. FLASH Cavity Gradient Stability Comparison of beam-off measurements of pulse-to-pulse cavity gradient jitter during the flattop.
Thickness of the Kamaboko Tunnel Shield Wall under Different Assumptions Ewan Paterson Technical Board June 23,
Andrew Moss ASTeC CM32 9t h February 2012 RAL MICE RF System.
Anders Sunesson RF Group ESS Accelerator Division
Klystron Cluster RF Distribution Scheme Chris Adolphsen Chris Nantista SLAC.
Marc Ross Nick Walker Akira Yamamoto ‘Overhead and Margin’ – an attempt to set standard terminology 10 Sept 2010 Overhead and Margin 1.
Power Distribution System R&D at SLAC Christopher Nantista ILC08 Chicago, Illinois November 18,
L-band (1.3 GHz) 5-Cell SW Cavity High Power Test Results Faya Wang, Chris Adolphsen SLAC National Accelerator Laboratory
KSC Operation Control of Cavity Gradients Failure Analysis Near and Long Term R&D Effect on Beam Emittance Chris Adolphsen SLAC 9/7/2010 Going Native in.
Christopher Nantista ILC10 Beijing, China March 27, 2010.
CLARA Gun Cavity Optimisation NVEC 05/06/2014 P. Goudket G. Burt, L. Cowie, J. McKenzie, B. Militsyn.
Linac RF Source Recommendations for Items 22,23,24,46,47 Chris Adolphsen.
Ding Sun and David Wildman Fermilab Accelerator Advisory Committee
ESS RF System Design Stephen Molloy RF Group ESS Accelerator Division SLHiPP2 4-May-2012.
Aug 23, 2006 Half Current Option: Impact on Linac Cost Chris Adolphsen With input from Mike Neubauer, Chris Nantista and Tom Peterson.
TE 01 -TE 02 DLDS Elements BINP-KEK
John Carwardine 21 st October 2010 TTF/FLASH 9mA studies: Main studies objectives for January 2011.
1 Update on Q2 Main linac starting gradient, upgrade gradient, and upgrade path Results of WG5 discussions after feedback from plenary on Tuesday New Option.
The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,
Evaluation of the TE 12 Mode in Circular Waveguides for Low-Loss High Power Transportation Sami G. Tantawi, C. Nantista K. Fant, G. Bowden, N. Kroll, and.
How CLIC-Zero can become less expensive A.Grudiev, D. Schulte 16/06/09.
KCS and RDR 10 Hz Operation Chris Adolphsen BAW2, SLAC 1/20/2011.
Global Design Effort - CFS Oct IWLC ML Single Tunnel Cross Section GDE Asian Regional Team KEK A. Enomoto.
KCS Main Waveguide Testing Chris Adolphsen Chris Nantista and Faya Wang LCWS12 Arlington, Texas October 25, 2012.
Jan Low Energy 10 Hz Operation in DRFS (Fukuda) (Fukuda) 1 Low Energy 10Hz Operation in DRFS S. Fukuda KEK.
SPL waveguide distribution system Components, configurations, potential problems D. Valuch, E. Ciapala, O. Brunner CERN AB/RF SPL collaboration meeting.
A Multi-Moded RF Delay Line Distribution System for the Next Linear Collider S. G. Tantawi, G. Bowden, Z.D. Farkas, J. Irwin, K. Ko, N. Kroll, T. Lavine,
HLRF R&D Towards the TDR Christopher Nantista ML-SCRF Webex meeting June 29, 2011.
Nextef status and expansion plans Shuji Matsumoto for KEK Nextef Group /5/51 4th X-band Structure Collaboration Meeting, CERN.
High-efficiency L-band klystron development for the CLIC Drive Beam High-efficiency L-band klystron development for the CLIC Drive Beam CLIC workshop,
Linac RF System Design Options Y. Kang RAD/SNS/NScD/ORNL Project – X Collaboration Meeting April , 2011.
A CW Linac scheme for CLIC drive beam acceleration. Hao Zha, Alexej Grudiev 07/06/2016.
ILC Power and Cooling VM Workshop
ILC High Power Distribution
A 6 GeV Compact X-ray FEL (CXFEL) Driven by an X-Band Linac
Klystron Cluster System (KCS)
A frequency choice for the SPL machine: Impact on hardware
Second SPL Collaboration Meeting, Vancouver May 2009
Chris Adolphsen Sergei Nagaitsev
Application of the moderate peak power (6 MW) X-band klystron’s cluster for the CLIC accelerating structures testing program. I. Syratchev.
12 GHz High Power RF components requirements for CEA activities
Update of CLIC accelerating structure design
CEPC RF Power Sources System
ATF project meeting, Feb KEK, Junji Urakawa Contents :
Presentation transcript:

KCS Operational Issues Chris Adolphsen, Chris Nantista and Faya Wang GDE PAC Review at KEK 12/12/12

 KCS + cryo shaft  KCS shaft e - beam e + beam undulator I.P main linac totals: 12 shafts 22 KCS systems 567 rf units ( ) 1,701 cryomodules 14,742 cavities RF power sources clustered in surface buildings. Power combined, transported through overmoded waveguide, and tapped off locally at each ML Unit. Two KCS systems per building/shaft feed upstream and downstream, ~1 km each. Klystron Cluster Scheme Shaft Layout and ML Units Powered

… Combine power from 19 klystrons – effectively a 190 MW klystron l … -3 dB -4.8 dB-7 dB dB 1 Combining and Tapping Off Power l dB -4.8 dB … … WC1890 CTO Tap-Off 10 MW every 38 m (three cryomodules)

Klystron to CTO Considered remote-controlled mechanical rf switches to isolate region upstream of CTO if circulators fail – removed to save cost CTO KLY Switch and Load 5 MW Circulator

RF Control Overview Have rf feedback loop to control net combined power from 19 klystrons Only need precise power summation when running at full beam energy Run klystrons in saturation and use alternating +phi/-phi phasing to control amplitude: phi nominally 22 deg to give 5% useable rf overhead Can shutoff rf at breakdown site with 7.4 us (propagation delay) RF Amplitude Phase (deg) Minimum Nominal

Prototype CTO’s built for R&D program. |E| on cut planes |H| on surfaces CTO (Coaxial Tap-Off) Coupling into the Circular Waveguide determines coupling To couple power to the pipe, developed a “coaxial (wrap-around) tap-off”, or CTO Couplings range from -3 dB to ~-14 dB are needed, controlled by gap width 3 dB design customized to coupling gap Coupling due to beating with TE 02

TE 01 TE 20 Electric field pattern TE 01 Main Waveguide: For low-loss and high power handling, the TE 01 mode is used in pressurized (3 bar N 2 ), copper-plated, overmoded, 0.48m-diameter circular waveguide (WC1890). Loss at this diameter = 8.44 %/km KCS Power Transmission Bends: 90  bends are needed to bring the KCS main waveguide to the linac tunnel. Mode converting sections allow the actual bending to be done in the rectangular TE 20 mode. WC1375 ports connect to WC1890 through step-tapers.

The 0.48m-diameter KCS Main Waveguide supports 20 parasitic modes. To avoid significant mode conversion losses, we set the radius tolerance at ~±0.5 mm. This was achieved within a factor of ~2. Because TM 11 is degenerate with TE 01, tilt (local and cumulative), should be kept within ~ 1  (17 mrad). The Q 0 for the 40 m resonant waveguide with CTO at one end and a bend at the other measured within 3.2% of the theoretical value! This is a good indication that mode conversion wasn’t a problem. target: mm mean: mm max-min: 1.08 mm std.: mm For the CTO and bend, fabrication tolerances were set at ~±127  m for critical dimensions and ~±178  m for concentricities. Our transmission tests with 2 CTO’s shorted for launching (not fine tuned) demonstrated ~98  99% transmission and a CTO match of ~-21  28 dB. KCS Tolerances Q 0, theor. = 187,230 Q 0, meas. = 181,310 For ILC, may tune CTO coupling after fabrication

into beam 16.8% not into beam 83.2% inefficiencies & losses 52.6% AC  RF 43.2% transmission losses 9.4% kly to ML unit: 6.8% LPDS: 2.6% into loads 30.6% operational 28.7% fill time: 21.4% beam phase: 0.31% LLRF overhead: 3.9% due to gradient spread 1.9% statistics: 0.61% unoptimized match: 1.3% KCS system (19 kly)Full Machine (413 kly) AC power2.764 MW60.08 MW lost above ground1.404 MW30.52 MW lost below ground0.895 MW19.45 MW into beam0.465 MW10.11 MW MW (83.2%) 16.8% KCS Losses

CTO cold tests Ten Meter Test Setup m m input assembly transmission tests resonant line tests Location: Roof of NLCTA bunker Power source: SNS modulator and Thales “5 MW” klystron

Forty Meter Test Setup CTO coupling RF power from P1 Marx-driven Toshiba MBK into TE 01 mode in resonant line using KEK circulator. 40 m of pressurized (30 psig), 0.48m diameter circular waveguide. Shorted bend with input mode converter at end of run. Recording run data.

|E s | pk = ~3.34 MV/m for 37.5 MW input (= 75 MW full geometry  300 MW TW equiv. at SW anti-nodes) Equivalent to 72 MW TW in WR650 ! Surface Electric Field in 90 Degree Bend

GHz f r = GHz (cold, unpress.) Q L = 78,839  = Q 0 = 181,310 Cold Test of 40 m Setup

First Run: 1 MW input (255 MW field equivalent – ILC needs only 190 MW initially), no breakdown in 120 hours with 1.6 ms pulses at 3 Hz

1.Coupling coefficient β = Power needed for equivalent field of 300 MW, Pin = 1.18 MW. Second Run: 1.25 MW input (313 MW field equivalent – ILC needs only 190 MW initially), one breakdown in 140 hours with 1.6 ms pulses at 3 Hz

Resonant Line 1.0 MW Equivalent Field for 300 MW Transmission 40 m of WC1890 back-shorted tap-in Resonant Ring 300 MW 80 m of WC1890 directional coupler In FY12: Installed 40 m of pipe system and bend prototype (have an additional unused 40 m of pipe) tap-off tap-in phase shifter In FYxx: Use resonant ring to test ‘final design’ bends and tap-in/off

Quantifying the CTO-to-CTO Reliability Want to verify that each 1.0 km CTO-to-CTO region either breaks down rarely (< 0.1/year) if the repair time is long (24 hours), or break downs modestly (< 1/day) if the recovery is quick (1 minute). For ILC – Power in tunnel (P) = Po*(L – z)/L, where z is distance from first feed and L = distance from first to last feed – RF shut off time (t) = (zo + z)*2.25/c where zo is the distance from the cluster to first feed – Max of P*t/Po = 3.2 us for zo = 100 m, L = 1.0 km – Max t = 7.4 us for zo = 100 m, L = 1.0 km For an 80 m resonant ring, t is at minimum equal to the rf roundtrip time = 0.33 us, so P*t would be at least ~ 1/10 of the max at ILC. Would need ~ 1 km of pipe and thee 10 MW klystrons to ensure the maximum energy absorption (P*t) of ILC – But it would be delivered at ~ twice the power in ~ half the time

Other Questions Modulator What is the plan to prove reliability of the Marx modulator design? We have not tested the P2 MARX enough to know where improvements need to be made. For the P1 Marx, the concern is still with the capacitor lifetime, but since we are focusing on the P2 and have little funds anyway, there is no further plans to develop the P1 or continue long-term testing it. How to find weak components in the design? We plan to do long term testing of the P2 starting next Feb. A large number of modulators operated at 5Hz would have an impact on the electrical grid. How is constant power consumption from the mains achieved ? The charging supply will present a constant load to the grid, so this should not be a problem What is the strategy for industrialization? We have been trying to find companies that will license the P2 design - Thompson showed some interest but have not followed up. Also, KEK has a DTI Marx modulator that they will evaluate - if it works well, maybe Toshiba or other companies will buy them

Other Questions (cont) Klystron: How is klystron lifetime defined? The expected klystron lifetime is based on the cathode loading - we have ran our MBK at 10 MW with ms pulses for 5000 hours at 5 Hz without major incident (except for the cavity detuning from a one-phase loss of AC power to the solenoid when the klystron beam was off), so at least we know the MBK lifetime is not very low - for either the KCS or DKS layout, there is no need to have a long lifetime other than cost since the klystrons are readily accessible if they fail. What is the plan to handle non-conforming klystrons during conditioning and testing, which takes place not at the manufacturers site? I would hope that the klystron contract would be such that the manufacturer would replace any non-conforming tubes as I believe the failure rate will be low

Other Questions (cont) Waveguide: What is the plan to prove reliability of the waveguide distribution system? We have already tested the rf distribution systems sent to FNAL at full power, but only for an hour or so. Hopefully, FNAL will be able to run them longer. There are some components which have sliding contacts, which seem to have poor reliability at high power. I believe only the U-bead phase shifters have the sliding contacts - they seem to work fine in the full power for the testing done so far (no breakdowns and no arcing damage observed) - note also that these shifters should not have to be adjusted often. Operation at overpressure might need approval by the national authorities ( TÜV or similar). This might lead to higher prices during the production process. Has that been considered? The waveguide has been designed for high pressure operation (and certified in most cases by the vendor) and costed accordingly. Unlike He systems, designing and qualifying for 3 atm absolute operation is not that difficult (e.g. to qualify our 40 m big pipe + bend + CTO, we pressurized system at 25% above design for a few hours).