FCC DUMP SYSTEM W. Bartmann, B. Goddard, R. Ostojic FCC Dump Meeting, 14 th Jan. 2015.

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Presentation transcript:

FCC DUMP SYSTEM W. Bartmann, B. Goddard, R. Ostojic FCC Dump Meeting, 14 th Jan. 2015

FCC-hh parameters 14-Jan-2015FCC dump layout 2

Basic assumptions on system concept – can change! Signal (trigger) from interlock system External dump block 2 dump systems (one per beam) Full beam extracted in one turn, with abort gap Fast kickers and septa to get out of ring lattice Absorber system (“dump block”) Dilution as needed – passive/active 14-Jan-2015FCC dump layout 3

FCC layout D. Schulte et al. 14/01/2015BTP in FCC, BTP Section Meeting 4

Rms sigma ~ 1 mm Assume otherwise max of 0.5 mm Quads of 4m length 500 T/m 400 m 100 m 110 m Extract the two beams from different straight sections Same plane deflections - or is Lambertson preferred? 14-Jan-2015FCC dump layout 5 Conventional dump design

Extraction trajectory – no bump MKE: 0.15 mrad 110 m drift Q5: 9 mm offset MSE: 35 mm offset at entrance 150 m drift to MSE 17 mm septum width 50 m for TCDQ 200 m for MSE 417 mm Q4 clearance 1.7 mrad, 284 T.m, 1.42 T 14-Jan-2015FCC dump layout 6

Extraction bump 14-Jan-2015FCC dump layout 7

Extraction trajectory with bump 14-Jan-2015FCC dump layout 8 MKE: 0.15  0.13 mrad 110 m drift Q5: 9 mm offset Bump: 9 mm 0.3 mrad  50 T.m 360 mm beam sep at bumper3 MSE: 35 mm offset at entrance 150 m drift to MSE 17 mm septum width 50 m for TCDQ+2 bumpers 200 m for MSE 417 mm Q4 clearance 1.7 mrad, 284 T.m, 1.42 T

14-Jan-2015FCC dump layout

SSC like Kicker still around quad Septum is part of the bump Region with better field quality used for circulating beam 2.0 mrad, 334 T.m Half of the central drift (~200) needed to reach beam separation at MSD entrance With 100 m of MSD not anymore NC Bumpers: 0.5 mrad, 84 T.m 14-Jan-2015FCC dump layout 10

SSC like - opening up central drift Without significantly increasing the max betas reach 500 m central drift With 100 m each side for bumpers and auxiliaries leave 300 m for septum 334T.m, 1.2 T  again NC Bumpers: 0.5  0.35 mrad, 60 T.m 14-Jan-2015FCC dump layout 11

HW parameters KickerSeptumBumpers B.dlT.m Available system lengthm Rise timeus10-- Flat top lengthus>340 GFR h/vmm18/18 14-Jan-2015FCC dump layout 12 Challenges: -Radiation hardness -Reliability -Kicker: energy range for switch design, limit in kA/s, peak current, impedance -Septum: overall system length, energy range, powering

Input for dump block and protection devices Dump material, shielding Dump line direction Dilution pattern, frequency Sweep pattern 14-Jan-2015FCC dump layout 13 Unit25 ns5 ns Bunch population1e110.2e11 # bunches Transv. emittance normalisedum Spotsize at dump (rms) for 1.5 km dump linemm – 0.7 Total beam energyGJ8.5 Average power (5 h fills)kW500

Machine protection, reliability,… Dump system reaction time Asynchronous dump survival Downstream (?) collimation system for ‘mopping up’ SIL level Radiation Fault tolerant/redundancy in design Self-tests and post-operational checks 14-Jan-2015FCC dump layout 14

Absorber “block”: ideas…. 10 m of low density graphite, with sweep/beta functions large enough to ensure remain below 10 kJ/g. Maybe kickers with SC dilution quads Some few 100 m of passive 'spoiler' to make the blow-up, e.g. few cm thick graphite plates, spaced by cm, to develop the shower with effectively low density - then a solid block of 10 m of graphite Ppressurised water dump, a la ILC (18 MW designed!), with low enough energy deposition and high enough pressure to avoid boiling the water locally....(difficult, as need to keep delta T to maybe a few hundred degrees!) Pressurised gas (N2?) dump, e.g m of N2 at 15 bar, which is the same amount of material as 10 m of graphite....issues of scattered losses in the pipe, pressure rise when it heats up, whether N2 stays N2 after a while, local plasma formation and creation of low pressure channel, etc. Solid block designed to melt, then resolidify when cold, e.g. lead, water (ice), Jan-2015FCC dump layout 15

Conclusions Assume dumps for the two beams in separated straights Extraction with kicker and septum around quad supported by bump 1.4 T for MSD  NC possible SSC like extraction Septum part of the bump  easier for field homogeneity If central drift is opened up to 500 m (betamax ~1100 m) MSD can be NC with ~1.2 T Septum not needed to extract the beam Dump block and protection devices Material (solid, liquid, gas), dilution, sweep pattern, … Machine protection Define reaction time, SIL level, fault tolerance, redundancy 14-Jan-2015FCC dump layout 16

Reference collection? Jan-2015FCC dump layout 17