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A Preliminary Look at the ILC Cryogenic System

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Title: A Preliminary Look at the ILC Cryogenic System


1
A Preliminary Look at the ILC Cryogenic System
  • Tom Peterson, Fermilab
  • ILC RD Meeting
  • 8 February 2006

2
ILC 500 layout
3
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4
ILC modules and cryogenic system are closely
based on the TESLA Technical Design Report (TDR)
  • TESLA TDR is available online (see references)
  • 9-cell niobium RF cavities at 1.3 GHz and 2
    Kelvin are the primary accelerating structures
  • Cavities are assembled into a cryostat called a
    cryomodule or module
  • ILC module concept is still the TDR module,
    except 8 cavities instead of 12 per module
  • TDR cryogenic system concept is retained

5
ILC cryogenic system effort is a very active
collaboration
  • CEA Grenoble, CERN, DESY, Fermilab, Jefferson
    Lab, KEK, SLAC
  • The concepts presented today represent the work
    of many people at these laboratories
  • Previous input from industry for the TESLA effort
    and for LHC is also important

6
1.3 GHz, 9 cell, Nb RF Cavity
7
TTF cryomodule
8
Module end
9
Generation 4, T4CM
10
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11
ILC cryogenic system overview (main linac)
  • Revising and resizing the TESLA cryogenic concept
  • Saturated He II cooled cavities _at_ 2 K
  • Helium gas thermal shield _at_ 5 - 8 K
  • Helium gas thermal shield _at_ 40 - 80 K
  • Two-phase line (liquid helium supply and
    concurrent vapor return) connects to each helium
    vessel
  • Two-phase line connects to gas return once per
    module
  • A small diameter warm-up/cool-down line connects
    the bottoms of the He vessels (primarily for
    warm-up)
  • Subcooled helium supply line connects to
    two-phase line via JT valve once per string (12
    modules)

12
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13
Sloped system concerns
  • Want heat removal without bubbling or boiling
  • Saturated superfluid heat flux limit about 1
    W/sq-cm
  • 54.9 mm dia down-pipe means 23.7 sq-cm or about
    24 W per cavity can be transferred away
  • But a claim was made that surface area limit is
    1/10 of that, 0.1 W/sq-cm, so 2.4 W/cavity limit
  • Hence, want to pool liquid in 2-phase pipe by
    means of dams in order to provide large surface
    area for evaporation
  • Conclusion in subsequent discussions -- dams not
    needed
  • Even just 2.4 W/cavity is enough, expect 1.7
    W/cavity at 36 MV/m
  • Most experience does not support the claim of the
    surface area heat flux limit
  • Sloped system should not be a problem, within
    limits
  • LHC will run some areas with 1.2 slope
  • DESY will test sloped modules for XFEL

14
Module heat estimates
15
Module predicted heat loads
16
Module pipe sizes increase
17
(Increase diameter beyond X-FEL)
(Increase diameter beyond X-FEL)
(Review 2-phase pipe size and effect of slope)
18
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19
Cryo-string
Now 12 cryomodules per string, totalling 140 m
20
Cryogenic unit 16 strings per cyrogenic unit,
so 192 modules per cryo unit (47 GeV)
21
CERN LHC capacity multipliers
  • Cryo capacity Fo x (Qd Qs x Fu)
  • Fo is overcapacity for control and off-design or
    off-optimum operation
  • Fu is uncertanty factor on load estimates, taken
    on static heat loads only
  • Qd is predicted dynamic heat load
  • Qs is predicted static heat load

22
Cryogenic unit parameters
23
Cryogenic unit length limitations
  • 25 KW total equivalent 4.5 K capacity
  • Heat exchanger sizes
  • Over-the-road sizes
  • Experience
  • Cryomodule piping pressure drops with 2 km
    distances
  • Cold compressor capacities
  • With 192 modules, we are hitting our plant size
    limits, cold compressor limits, and pressure drop
    limits

24
Cryogenic unit segmentation and other cryogenic
boxes
  • Segmentation issue is ultimately tied to
    reliability
  • BCD should include features for vacuum
    segmentation
  • Assume 4 cryo strings (48 modules, 563 meters)
    per segmentation unit
  • Cryogenic string supply and end boxes, which may
    (should!) be separate from modules, are also
    required within the ILC lattice

25
Full segmentation concept (ACD)
  • A box of slot length equal to one module
  • Can pass through cryogens or act as turnaround
    box from either side
  • Does not pass through 2-phase flow, so must act
    as a supply or end of a cryogenic string
  • Includes vacuum breaks
  • May contain bayonet/U-tube connections between
    upstream and downstream for positive isolation
  • May contain warm section of beam pipe
  • May also want external transfer line for 4 K
    standby operation (4 K only, no pumping line)

26
Lengths and packing factor (from spreadsheet
originated by Chris Adolphsen and revised by Tom
P.)
27
Cryogenic unit packing factor
  • About 0.7 active RF length/total length
  • Cryo boxes can be very short along the length of
    the linac if they have appendages to the side for
    valves, heat exchangers, liquid helium
    reserviors, etc. But these then require alcoves.
    Is this better than running the TBM slightly
    further?
  • Cryo boxes can be incorporated into modules,
    improving the packing factor, but creating dozens
    of odd and special modules. (We are keeping
    cryogenic boxes separate.)

28
ILC 500 cryogenic system overview for main linacs
  • 10 large cryogenic plants (5 per linac)
  • Approximately 2.3 km unit lengths
  • Each cryogenic plant of about the maximum size --
    equivalent to about 25 kW at 4.5 K
  • Each plant about 5.2 MW wall plug power
  • ILC 500 main linac cryogenics about 52 MW total

29
ILC cryogenics is more than these main linac
cryogenic units
  • ILC will have many other cold devices other than
    these regular linear patterns of main linac
    cryogenic modules
  • Most work so far has focused just on a simplified
    view of the main linac cryogenics

30
Cold devices
  • 940 main linac modules per 250 GeV linac (so 940
    x 2)
  • Pre-accelerators up to 5 GeV (2 of these)
  • 10 special low-energy magnet/RF modules (x 2)
  • 61 standard modules, equiv to 5 strings (x 2)
  • Damping rings (1 electron, 2 positron)
  • Electron side -- 650 MHz SRF, about 15 cavities
    plus 200 m of CESR-c type SC wigglers 1200 W
    total at 4.5 K
  • Positron side -- 650 MHz SRF, about 10 cavities
    plus 200 m of CESR-c type SC wigglers x 2 rings
    2000 W total at 4.5 K
  • 200 meters of SC undulators in electron linac
    (300 W)
  • SC magnets and crab cavities in interaction
    regions
  • Various cryogenic feed, end, and transition boxes
  • Several km of cryogenic transfer lines

31
BCD Description -500 GeV Layout- (Slide lifted
from Positron Source Configuration by KURIKI
Masao and John Sheppard, January 2006.Cryogenic
device description in red added by Tom Peterson)
Up to about 500 MeV via special SRF cavity/magnet
modules totaling about 25 m x 20 MV/m Then up to
5 GeV with 21 standard SRF modules
650 MHz SRF, about 10-15 cavities plus 200 m of
CESR-c type SC wigglers, all 3 damping rings
SC magnets and crab cavities (no
quatities yet)
Standard modules (starting at 5 GeV)
Standard modules
RTML includes SC solenoids plus 61 SRF modules
RTML includes SC solenoids plus 61 SRF modules
200 m of SC undulators
Up to about 500 MeV via special SRF cavity/magnet
modules totaling about 25 m x 20 MV/m Then up to
5 GeV with 21 standard SRF modules
32
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33
Cryogenic system intertwined with linac lattice
and conventional facilities
  • For example, warm beam tube sections could go
    into segmentation boxes
  • Conversely, we would try to locate breaks in
    the cryogenic system at interruptions in the
    lattice
  • Some flexibility with respect to unit lengths and
    segmentation lengths
  • RF unit of 3 modules should not be broken
  • Prefer to keep cryo strings (12 modules)
    unbroken, but a 9 or 15 module string is possible
  • Can try to locate plants at other above-ground
    facilities

34
ILC cryogenic system inventory
Since we have not counted all the cryogenic
subsystems and storage yet, ILC probably ends up
with a bit more inventory than LHC
35
Cryoplant concept
36
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37
Size comparison to TESLA TDR
  • TESLA 500 TDR had 7 large cryoplants
  • 5 at about 5.2 MW and 2 smaller
  • ILC 500 looks like about 12 large cryoplants
  • 10 at about 5.2 MW and 2 smaller
  • Dynamic load up with gradient squared (length
    reduced by gradient), larger multipliers, lower
    plant efficiency
  • Costs increase roughly linearly with increasing
    cryoplant power when we are pegged at the 25 KW
    plant size.
  • Increased heat means adding plants, shortening
    strings, etc., so not the 0.6 or 0.7 power
    correlation with power at these levels of load.

38
ILC cryogenics -- open issues
  • Cryogenic loads outside of the main linac
    cryomodule strings (magnets, DR RF, etc.)
  • Multiplier factors for sizing system
  • High flow rates (about 50 times TTF flows)
  • Segmentation philosophy (minimal or more)
  • Reliability estimates
  • Trustworthy predictions for module strings will
    require more experience with this technology
  • LHC experience will tell a lot about reliability
    of a large-scale 2 K cryogenic system similar to
    ILC
  • Upgrade heat loads and scenarios
  • At 35 MV/m estimate 50 more heating

39
References
  • TESLA TDR -- online as TESLA Report 2001-23 at
    http//tesla.desy.de/new_pages/TESLA/TTFnot01.html
  • Navigate to other TESLA and TTF documents going
    back to 1993 from the same web page
  • ILC BCD documents
  • http//www.linearcollider.org/wiki/doku.php?idbcd
    bcd_home
  • bcdmain_linacilc_bcd_cryogenic_chapter_v3.doc
  • ILC presentations
  • Navigate from ILC home page via Calendar/Past
    Events and Calendar/GDE Meetings
  • http//www.linearcollider.org/cms/?pid1000012
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