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Chronological Thread  
  • From: "Kistenev, Edouard" <kistenev AT bnl.gov>
  • To: "Haggerty, John" <haggerty AT bnl.gov>, "Lajoie, John G [PHYSA]" <lajoie AT iastate.edu>
  • Cc: "sphenix-hcal-l AT lists.bnl.gov" <sphenix-hcal-l AT lists.bnl.gov>
  • Subject: Re: [Sphenix-hcal-l] iHCAL thermal testing
  • Date: Wed, 6 Jan 2021 17:07:48 +0000

John, 
you really made me worried - I was under impression that we are not planning to make IHCal a heat sink for every heat source around. It will not work. My assumption always been the air is flowing in the space between EMC and IHCal and probably even between IHCal and solenoid. Al is too good a heat conductor for IHCal to be left to its own defenses. Some information answering my questions is enclosed. To some extent it may also explain high temperature in 1/11 area (if I read the numbering correctly). 

Edward


One can find even better compilation at 
https://www.engineersedge.com/properties_of_metals.htm


Al is much more conductive compared to steel of many other "choice" materials for calorimetry - almost transparent. 
Metal, Metallic Element or Alloy Temperature
- t - 
(oC)

Thermal Conductivity 
- k - 
(W/m K)
Aluminum -73 237
" 0 236
" 127 240
" 327 232
" 527 220
Aluminum - Duralumin (94-96% Al, 3-5% Cu, trace Mg) 20 164
Aluminum - Silumin (87% Al, 13% Si) 20 164
Aluminum bronze 0 - 25 70
Aluminum alloy 3003, rolled 0 - 25 190
Aluminum alloy 2014. annealed 0 - 25 190
Aluminum alloy 360 0 - 25 150
Antimony -73 30.2
" 0 25.5
" 127 21.2
" 327 18.2
" 527 16.8
Beryllium -73 301
" 0 218
" 127 161
" 327 126
" 527 107
" 727 89
" 927 73
Beryllium copper 25 0 - 25 80
Bismuth -73 9.7
" 0 8.2
Boron -73 52.5
" 0 31.7
" 127 18.7
" 327 11.3
" 527 8.1
" 727 6.3
" 927 5.2
Cadmium -73 99.3
" 0 97.5
" 127 94.7
Cesium -73 36.8
" 0 36.1
Chromium -73 111
" 0 94.8
" 127 87.3
" 327 80.5
" 527 71.3
" 727 65.3
" 927 62.4
Cobalt -73 122
" 0 104
" 127 84.8
Copper -73 413
" 0 401
" 127 392
" 327 383
" 527 371
" 727 357
" 927 342
Copper, electrolytic (ETP) 0 - 25 390
Copper - Admiralty Brass 20 111
Copper - Aluminum Bronze (95% Cu, 5% Al) 20 83
Copper - Bronze (75% Cu, 25% Sn) 20 26
Copper - Brass (Yellow Brass) (70% Cu, 30% Zn) 20 111
Copper - Cartridge brass (UNS C26000) 20 120
Copper - Constantan  (60% Cu, 40% Ni) 20 22.7
Copper - German Silver (62% Cu, 15% Ni, 22% Zn) 20 24.9
Copper - Phosphor bronze (10% Sn, UNS C52400) 20 50
Copper - Red Brass (85% Cu, 9% Sn, 6%Zn) 20 61
Cupronickel 20 29
Germanium -73 96.8
" 0 66.7
" 127 43.2
" 327 27.3
" 527 19.8
" 727 17.4
" 927 17.4
Gold -73 327
" 0 318
" 127 312
" 327 304
" 527 292
" 727 278
" 927 262
Hafnium -73 24.4
" 0 23.3
" 127 22.3
" 327 21.3
" 527 20.8
" 727 20.7
" 927 20.9
Hastelloy C 0 - 25 12
Inconel 21 - 100 15
Incoloy 0 – 100 12
Indium -73 89.7
" 0 83.7
" 127 75.5
Iridium -73 153
" 0 148
" 127 144
" 327 138
" 527 132
" 727 126
" 927 120
Iron -73 94
" 0 83.5
" 127 69.4
" 327 54.7
" 527 43.3
" 727 32.6
" 927 28.2
Iron - Cast 20 52
Iron - Nodular pearlitic 100 31
Iron - Wrought 20 59
Lead -73 36.6
" 0 35.5
" 127 33.8
" 327 31.2
Chemical lead 0 - 25 35
Antimonial lead (hard lead) 0 - 25 30
Lithium -73 88.1
" 0 79.2
" 127 72.1
Magnesium -73 159
" 0 157
" 127 153
" 327 149
" 527 146
Magnesium alloy AZ31B 0 - 25 100
Manganese -73 7.17
" 0 7.68
Mercury -73 28.9
Molybdenum -73 143
" 0 139
" 127 134
" 327 126
" 527 118
" 727 112
" 927 105
Monel 0 – 100 26
Nickel -73 106
" 0 94
" 127 80.1
" 327 65.5
" 527 67.4
" 727 71.8
" 927 76.1
Nickel - Wrought 0 – 100 61 – 90
Cupronickel 50 -45 (Constantan) 0 - 25 20
Niobium (Columbium) -73 52.6
" 0 53.3
" 127 55.2
" 327 58.2
" 527 61.3
" 727 64.4
" 927 67.5
Osmium 20 61
Palladium 75.5
Platinum -73 72.4
" 0 71.5
" 127 71.6
" 327 73.0
" 527 75.5
" 727 78.6
" 927 82.6
Plutonium 20 8.0
Potassium -73 104
" 0 104
" 127 52
Red brass 0 - 25 160
Rhenium -73 51
" 0 48.6
" 127 46.1
" 327 44.2
" 527 44.1
" 727 44.6
" 927 45.7
Rhodium -73 154
" 0 151
" 127 146
" 327 136
" 527 127
" 727 121
" 927 115
Rubidium -73 58.9
" 0 58.3
Selenium 20 0.52
Silicon -73 264
" 0 168
" 127 98.9
" 327 61.9
" 527 42.2
" 727 31.2
" 927 25.7
Silver -73 403
" 0 428
" 127 420
" 327 405
" 527 389
" 727 374
" 927 358
Sodium -73 138
" 0 135
Solder 50 - 50 0 - 25 50
Steel - Carbon, 0.5% C 20 54
Steel - Carbon, 1% C 20 43
Steel - Carbon, 1.5% C 20 36
" 400 36
" 122 33
Steel - Chrome, 1% Cr 20 61
Steel - Chrome, 5% Cr 20 40
Steel - Chrome, 10% Cr 20 31
Steel - Chrome Nickel, 15% Cr, 10% Ni 20 19
Steel - Chrome Nickel, 20% Cr, 15% Ni 20 15.1
Steel - Hastelloy B 20 10
Steel - Hastelloy C 21 8.7
Steel - Nickel, 10% Ni 20 26
Steel - Nickel, 20% Ni 20 19
Steel - Nickel, 40% Ni 20 10
Steel - Nickel, 60% Ni 20 19
Steel - Nickel Chrome, 80% Ni, 15% Ni 20 17
Steel - Nickel Chrome, 40% Ni, 15% Ni 20 11.6
Steel - Manganese, 1% Mn 20 50
Steel - Stainless, Type 304 20 14.4
Steel - Stainless, Type 347 20 14.3
Steel - Tungsten, 1% W 20 66
Steel - Wrought Carbon 0 59
Tantalum -73 57.5
" 0 57.4
" 127 57.8
" 327 58.9
" 527 59.4
" 727 60.2
" 927 61
Thorium 20 42
Tin -73 73.3
" 0 68.2
" 127 62.2
Titanium -73 24.5
" 0 22.4
" 127 20.4
" 327 19.4
" 527 19.7
" 727 20.7
" 927 22
Tungsten -73 197
" 0 182
" 127 162
" 327 139
" 527 128
" 727 121
" 927 115
Uranium -73 25.1
" 0 27
" 127 29.6
" 327 34
" 527 38.8
" 727 43.9
" 927 49
Vanadium -73 31.5
" 0 31.3
" 427 32.1
" 327 34.2
" 527 36.3
" 727 38.6
" 927 41.2
Zinc -73 123
" 0 122
" 127 116
" 327 105
Zirconium -73 25.2
" 0 23.2
" 127 21.6
" 327 20.7
" 527 21.6
" 727 23.7
" 927 25.7

Alloys - Temperature and Thermal Conductivity

Temperature and thermal conductivity for 

  • Hastelloy A
  • Inconel
  • Nichrome V
  • Kovar
  • Advance
  • Monel

alloys:

Alloys - temperature and thermal conductivity - Hastelloy A, Inconel, Nichrome V, Kovar, Advance, Monel




From: sPHENIX-HCal-l <sphenix-hcal-l-bounces AT lists.bnl.gov> on behalf of John Haggerty <haggerty AT bnl.gov>
Sent: Wednesday, January 6, 2021 11:48 AM
To: Lajoie, John G [PHYSA] <lajoie AT iastate.edu>
Cc: sphenix-hcal-l AT lists.bnl.gov <sphenix-hcal-l AT lists.bnl.gov>
Subject: Re: [Sphenix-hcal-l] iHCAL thermal testing
 
John et al.,

Sorry I couldn't stay to discuss this but here are a few more comments
based on what I did hear:

Things to do next:

1- make sure all the preamps are actually powered and reading their
thermistors
2- make sure the preamp thermistors are actually attached somewhere we
want to know the temperature
3- stick a temperature sensor on the hottest IB component (I guess
that's the LDO)
4- take another couple hours of data

I'm not sure whether it makes sense to try to thermally isolate the
sector completely from the environment, we should kick this around a bit
more, and I'll talk to Rob about it; he has a good feeling for thermal
issues.

I'm no expert on thermal management, but I've played around with things
like this:

> https://www.powerstream.com/temperature-rise-in-an-electronics-enclosure.htm

to see if what we observe seems consistent with what we expect, and it
seems to me to make sense to provide an air inlet so we have a
controlled way for air to enter the sectors rather than relying on
random leaks.  I think the only way we could do better would be to
thermally attach the interface board to a cooling plate which would be
in thermal contact with the sector structure (making the entire IHCAL
the heat sink), but I sort of doubt it's warranted based on what we've
seen so far.

Edward asked about the pattern of temperatures, which I think does not
measure what we want to know, because I'm not sure what the thermistors
are in contact with (air? aluminum? the preamp?), so I would not draw
any conclusions without another test (which will also have more of
them).  I should add that trying to get excellent and long-lived thermal
contact to thermocouples or thermistors is not so easy; glue tends to
give way, the sensors are small, and it's not so easy to get the SiPM
temperatures even in the EMCAL, and it's harder in the HCAL.

I think there is no path to cooling the SiPM's, so we're going to have
to learn to live with the noise at room temperature, which is less good
for the IHCAL the the OHCAL, since the neutron dose is less than the
emcal according to Jin's simulation, but it's not order of magnitude
less like the OHCAL, but we can only do what we can do.

On 2021-01-05 15:33, Lajoie, John G [PHYSA] wrote:
> Hi John H,
>
> Thanks for showing the slides on the iHCAL thermal tests today, it's
> great to get that rolling. It makes sense that you see temperatures
> similar to the oHCAL sectors.
>
> What I am having a hard time getting my brain around is what sort of
> tests we have to do to convince ourselves that we are OK, and whether
> or not the thermal solution that has been designed for the iHCAL is
> adequate (or needed?).  As I see it there are two things we need to
> address:
>
> - The LDO's on the boards at the end of the sector don't like to get
> too hot. I think you saw a 60C peak? Obviously with the colling tube
> and vanes in the bay that will help somewhat but can we put a
> thermistor on the LDO's?
>
> - The iHCAL is in a different situation than the oHCAL. The oHCAL can
> just radiate all it's heat out the back, while the iHCAL is sandwiched
> between the EMCal and the cryostat.  A standalone sector test that
> shows temperatures similar to the oHCAL is fine, but what happens when
> it is installed? I really don't know how to answer this question. It
> may be that all the heat is transferred to the frame and exits though
> the end rings, but I'd feel more comfortable with an expert telling me
> that was a valid assumption.  In particular I don't want to find we
> present some sort of heat load to the cryostat.
>
> I absolutely do NOT want to over complicate the iHCAL thermal testing.
> Before we go further, is there some additional expertise at BNL that
> we could tap into to sanity check our approach?  If we could get some
> input that would better define the key tests we have to do we could
> save a lot of time.
>
> Regards,
>
> John
>
> John Lajoie
>
> he, him, his
>
> Professor of Physics
>
> Iowa State University
>
> (515) 294-6952
>
> lajoie AT iastate.edu

---
John Haggerty
haggerty AT bnl.gov
cell: 631 741 3358
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