ess-bilbao initiative workshop. psi experience with high power beam handling, activation and...
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PSI experience with high power beam handling, activation and radiation protection.Mike Seidel (PSI).TRANSCRIPT
PAUL SCHERRER INSTITUT
PSI experience with high power beam handling, activation and radiation protection
M.Seidel, PSIESS - Bilbao Initiative Workshop, March 16-18, 2009
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
Outline� the PSI facility and its performance[overview, cyclotrons, availability, resonators, target]
� intensity limiting effects[space charge and beam blow up, scaling law for cyclotrons, round
beam, beam dynamics simulations]
� high power related accelerator aspects[special controls/diagnostics, interlock systems, shielded beamlines,
activation]
� specific infrastructure[rad.safety, disposal, legal requirements and all that …]
� conclusion
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
Injector II Cyclotron 72 MeV
870 keV transfer channel
72 MeV transfer channelRing Cyclotron 590 MeV
SINQ transfer channel
SINQspallation source
Overview PSI Facility
2.2 mA /1.3 MW
1.5 mA /0.9 MWCW operation
isotope production(Ib <100µµµµA)
µµµµ/ππππ secondary beamlines
target M (d = 5mm)
target E (d = 4cm)
Cockcroft Walton
proton therapie center [250MeV sc. cyclotron]
SINQexperiments
[Markus Lüthy]
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
TASPRITA-II
TRICS POLDI MORPHEUS AMOR
FOCUS
SANS-I
SANS-II
HRPT
DMC
NEUTRA
CNR
MARS
Eiger
K. ClausenSpallation Source Experimental Area – 13 Beamlines
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
CW Acceleration using a Sector Cyclotron
590 MeV Ring Cyclotron(magnets) in operation for 30+ years
- 8 Sector Magnets 1 T- Magnet weight ~250 tons- 4 Accelerator Cavities850kV (1.2MV)- Accelerator frequency: 50.63 MHz- harmonic number: 6- beam energy: 72 →→→→ 590MeV- beam current max.: 2.2 mA- extraction orbit radius: 4.5m
- relative Losses @ 2mA: ~1..2⋅⋅⋅⋅10-4
- transmitted power: 0.26-0.39 MW/Res.
Pro: Con:
- CW operation is inherently stable - inj./extr. difficult, interruptions, losses!
- efficient power transfer with only 4 resonators - large and heavy magnets (therm. equiliblium!)
- cost effective, compact - energy limited ~1GeV
[- no pulsed stress in target] [- no pulsed structure for neutrons]
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
history max. current of the PSI accelerator
license temporary operation with 2.2mA given
4 Cu Resonators complete
beam current is limited by beam losses;
upgrade path foresees constant absolute losses by improvements of the accelerator
1.3MW !
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
reliability and trips
duration of interruption ~30sec
duration of run period (this case: 21hours!)
� typical: short (30sec) interrupts; trips of electrostatic elements; loss interlocks� average availability: 90%; from June to December 2008: 94%(!)� on average: 25 trips per day
in the discussion on application of cyclotrons for ADS systemsthe frequency of interruptions is of major interest
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
major component: RF Resonators for Ring Cyclotron
• the shown Cu Resonators have replaced the original Al resonators [less wall losses, higher gap voltage possible, better cooling distribution, better vacuum seals]
• f = 50.6MHz; Q0 = 4⋅⋅⋅⋅104; Umax=1.2MV (presently 0.85MV→186 turns in cyclotron, goal for 3mA: 165 turns)
• transfer of up to 400kW power to the beam per cavity• deformation from air pressure ~20mm; hydraulic tuning devices in feedback
loop → regulation precision ~10µm
hydraulic tuning devices (5x)
resonator inside
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
historical development of turn numbers in PSI Ring Cyclotron
Cyclotron Facility Upgrade Path• keep absolute losses constant; increase acceleration
voltage and beam quality, better turn separation at extraction
• losses ∝ [turns]3 ∝ [charge density (sector model)] × [accel. time] / [turn separation] (W.Joho)
turns Ring turns Injector
now (2.0mA)
202(Upeak≈3.0MV)
81(Upeak≈1.12MV)
inter. step(2.6mA)
~180(Upeak≈3.3MV)
~73(Upeak≈1.25MV)
upgrade(3.0mA)
~165(Upeak≈3.6MV)
~65(Upeak≈1.40MV)
planned turn numbers and voltages
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
critical: electrostatic elements
principle of extraction channel
injection element in Ring
Tungsten stripesbeam pattern on outer turns in Ring
parameters extraction chan.:Ek= 590MeVE = 8.8 MV/mθ = 8.2 mradρ = 115 mU = 144 kV
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
extraction losses reduced by faster acceleration
achieved in 2008:
gap voltage increase: 780kV → 850kV
turn number reduction: 202 → 186
figure shows absolute losses for optimized machine setup
absolute loss (nA) in Ring Cyclotron as a function of current
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
avoid tail generation with short bunches
-multiparticle simulations-106 macroparticles [on supercomputer simulation of all protons in bunch feasible!]
- precise field-map- bunch dimensions: σσσσz ~ 2, 6, 10 mm; σxy ~ 10 mm
→ operation with short bunches and reduced flattop voltage seems possible
numerical study of beam dynamics in Ring Cyclotron
→ behavior of short bunches, generated by 10’th harmonic buncher
→ optimum parameters of flat-top cavity at these conditions
court.: J.Yang CAEA
radial/long. bunch distribution, varying initial bunch length
after 100 turns!
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
“round beam” – space charge in cyclotrons
qualitative picture:
protons in the field of a round, short bunch + vertically oriented magnetic field (neglect relativistic effects and focusing)
[Chasman & Baltz (1984)]
though the force is repulsive a “bound motion” is established
→ for short bunches a round beam shape is formed
coordinate frame moves with bunch
→ a round beam is observed in the Injector II cyclotron
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
High Power Meson Production Target
p-beam
BALL BEARINGS *)Silicon nitride ballsRings and cage silver coatedLifetime 2 y*) GMN, Nürnberg, Germany
SPOKES
To enable the thermal expansion of the target cone
TARGET CONE
3.0mA o.k., limit: sublimation
Mean diameter: 450 mmGraphite density: 1.8 g/cm3
Operating Temp.: 1700 KIrrad. damage rate: 0.1 dpa/AhRotation Speed: 1 Turn/sTarget thickness: 60 / 40 mm
10 / 7 g/cm2
Beam loss: 18 / 12 %Power deposit.: 30 / 20 kW/mA
G.Heidenreich et. al.
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
high power beams – technical safetybeam hits material (e.g. steel vacuum chamber):
K/sec000.250]g/cm[2 2
0 =≈∆∆
pIyx cP
tT
λσσπ
beam power
beam size material specific interaction length
heat capacity
melts after 8ms !
→ fast and reliable interlock systems are necessary to avoid damage !
[even more so in pulsed machines with higher P0]
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M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
Diagnostics for Machine Protection
→→→→ losses outside margins are interlocked (including low values)
System based on ca. 150 interconnected very fast (<100µs) hardware CAMACand VME modules treating about 1500 signals provided by the equipment:
1. Ionisation chambers as beam loss monitors with fixed warning and interlock limits; critical ones also with limits as function of the beam current.Simple and reliable device
Permanent display of losses
Warning level
Actual losses
Dyamic window
log
scal
e
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
Diagnostics (cont.)2. Segmented Collimators measuring the balance of right and left, up and down
scraped beam currents
� interlock is generated in case currents or asymmetry of currentsexceeds margin
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
Diagnostics (cont.)3. Beam current transmission monitors compare the beam current at different
spots for detecting loss of beam, normally 100% of transmission except at the targets and when beams are splitted.
100 % transmission in main cyclotron
100 % transmission in beampipes, except for splitted beams
97 % transmission of thin target M
70 % transmission of thick target E
Integration time:110 ms at 0 µA down to 10 ms above 1.5 mAWindow:± 5 µA at 0 µA and ± 90 µA at 2 mA
4. Many other signals: validity window on magnet settings, cavity voltages, …
transmission monitoring through Meson production target E
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
practical experience: overheating of Lead filled steel tubes in spallation target because of wrong beam optics
� cause: wrong beam optics installed, caused narrow beam width →→→→ power density too high
� usual current density <=40µA/cm2, in this case: 70µA/cm2
Pb filled stainless steel tubes
Pb filled Zy-2 tubes
Target cooling
Window cooling
neutron radiography
damaged tubes
wrong beam optics (pink), matched for 6cm Meson target but accidentally applied for 4cm target
note: βγεβγεβγεβγεx = 7.5/40 mm⋅⋅⋅⋅mrad before/after 4cm graphite target
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
special interlock system: direct current density monitoring
beam projection on a glowing mesh observed with an optical camera; problem: lifetime of camera; new version: glass-fiber optics to shielded camera position
2d display and projection
metallic mesh (tungsten)
vertical cut through beamline and target showing installation of VIMOS camera
VIMOS, K.Thomsen
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
Shielding� strategy: use standardized (mobile) concrete/iron blocks for shielding purposes� in PSI experimental hall: totally ~10.000 shielding blocks; in sum 32.000 tons of
weight; all documented in CATIA CAD system� iron is 30% fraction by the number� 14 different standardized shapes� 20% per the number of the blocks have special shapes with odd dimensions
PSI experimental hall
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
BEAM DUMP
shielding (2) – target / 590MeV transport chan.
side view
primary shielding
Iron !
vacuum chimneys for inserts, pumping connections
� elaborate shielding required
� reliability of activated components!; water cooling; few electrical connections
Component activation in beamline up to ~300Sv/h!
secondary shielding
platform for electronics, pumps etc.
collimators
4cm TargetBeam Dump
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
predicted activation at Meson production target
D.Kiselev, M.Wohlmuther
30% beam loss; target (1..3Sv/h) exchange via special flask
top view
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
activation level allows for necessary service/repair work• personnel dose for typical repair mission 50-300µSv• optimization by adapted local shielding measures; shielded service boxes for
exchange of activated components• detailed planning of shutdown work
activation map of Ring Cyclotron
(EEC = electrostatic extraction channel)
personal dose for 3 month shutdown (2008):
57mSv, 188 persons max: 2.6mSv
cool down times for service:
2000 → 1700 µA for 2h
0 µA for 2h
map interpolated from ~30 measured locations
measured component activation – Ring Cyclotron
EEC
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
overview: auxiliary expertise for High Power Operation
High Power Accelerator
Facility
Personnel Safety Systems
[access to accelerator bunkers, experimental
areas]
technical infrastructure[vacuum, cooling, RF, magnets,
power supplies, survey, diagnostics, controls etc.]
Radiative Waste Disposal
[declare nuclide inventory, predict disposal costs,
simulate temporary storage decay etc]
Facility Licensing [documentation and
paperwork, communication with legal authorities]
Radiation Safety
[personnel dose monitoring, radiation
monitoring etc.]
specific infrastructure[HotLab, mobile shielding
devices, radioanalytics etc.]
technical safety systems[interlock systems]
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
special infrastructure – hot cell facility
view through lead-glass window:
Meson production target wheel
irradiated SINQ spallation target, taken out of the cover
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
• mobile and specifically adapted shielding devices are used for targets and critical components as extraction elements or septum magnets
• target exchange flasks are complicated and expensive devices [heavy, motors, instrumentation, SPS controls]
special infrastructure – mobile shielding / exchange flask
picture: exchange flask for Meson production target E (4cm graphite wheel)
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
numerical modelling in the context of high power beams
particle generation/transport without/with electromagnetic fields
MCNPX, MARS
activation of components PWWMBS, MCNPX
radioactive waste disposal, declaration of nuclide inventory
PWWMBS, ISRAM
design/estimation of shielding MCNPX, ATTILA
thermo hydraulic / cooling problems ANSYS, CFD-ACE
beam dynamics codes omitted here!
Activity [Bq]
1.E+00
1.E+02
1.E+04
1.E+06
1.E+08
1.E+10
1.E+12
1.E+14
Fe-55
Co-60 H-3
Ni-63
Ti-44
Mn-54
Ni-59
Na-22
Zn-65
Ag-10
8mC-1
4Mo-
93Cl-3
6Fe-
60Be-
10
Bq
example: predicted nuclide inventory for old beam dump
M.WohlmutherS.TeichmannD.Kiselev
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
Summary
• the PSI accelerator delivers 1.3MW beam power in continuous mode; average reliability is 90%; ~25 trips per day
• performance is limited by uncontrolled losses →upgrade path through faster acceleration (higher resonator voltages) + bunch compression; max. acceptable activation of serviced accelerator components: ~ several mSv; total loss ~ 200W
• infrastructure for dealing with activated components and formal aspects connected to safety and radiation issues are challenging and are often underestimated!
M.Seidel, ESS Bilbao Initiative Workshop, March 16-18 (2009)
Thank you for your attention!