Superconducting Technology Assessment - nitrd
Superconducting Technology Assessment - nitrd
Superconducting Technology Assessment - nitrd
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Several issues need to be resolved for working SCE systems. Modularity and assembly sequence are the most<br />
important issues for larger scale systems. Other major technical issues include the penetration of vacuum walls and<br />
shields with multitude of both low- and high-frequency cable, concurrent presence of high DC current and very<br />
high frequencies (50-100 GHz) digital signals and the thermal gradient from room temperature to 4 K and the<br />
resulting material compatibility requirements. The packaging is also a very strong function of the IO approach used<br />
to bring high data rate signals into and out of the SCE circuits. If optical data transfer is selected, the fibers and<br />
other OEO components represent an additional class of materials that may complicate system integration. Due to<br />
the lack of a previous design at large scale (e.g., a functional teraflop SCE supercomputer), other potential issues<br />
may be hidden and can only be discovered when such an engineering exercise takes place. The past funding<br />
(commercial and government) for the development of such systems was in disconnected increments that prevented<br />
the accumulation of engineering now-how. Therefore, substantial learning and more development is needed to<br />
insure a functional SCE-based supercomputer system.<br />
Cooling<br />
An SCE-circuit-based system needs to operate at temperatures ranging from 4 to 77 K. The cooling is performed by<br />
using cryocoolers or by liquid cooling using refrigerants such as Liquid Helium (LHe) or Liquid Nitrogen (LN 2). Liquid cooling:<br />
■ Often produces a smaller temperature gradient between the active devices and the heat sink than<br />
in vacuum cooling, making it easier to bias all the chips at their optimum design temperature.<br />
■ Also produces a more stable bias temperature due to the heat capacity of the liquid that tends<br />
to damp any temperature swings produced by the cooler, often allowing liquid cooled devices<br />
to perform better than in vacuum mounted parts.<br />
For safety and practical reasons, liquid cooling is limited to 4 K (LHe) and 77 K (LN2) regions. Liquid cooling which<br />
fails to recondense the evolved gas is not suitable for large scale devices, but closed systems with liquifiers are well<br />
established in the particle accelerator community where total cooling loads are large and direct emersion of parts<br />
into boiling cryogen is straightforward. Additionally, the boiled-off working fluid can be used to cool electrical leads<br />
going into the device, although this means they must be routed thru the vacuum vessel with the gas for some<br />
distance which may be unduly constraining. Small closed cycle coolers commonly use helium gas as a working fluid<br />
to cool cold plates to which the circuits are mounted in vacuum. By using mixed gases and other means, the<br />
temperatures of intermediate temperature stages can readily be adjusted. The most common type of small<br />
cryocoolers in the marketplace are the Gifford McMahon (GM) type cryocooler, but pulse tube coolers and Stirling cycle<br />
refrigerators which offer lower vibration and maintenance and better efficiency at a currently higher cost are also used.<br />
In selecting the cooling approach for systems, the heat load at the lowest temperatures is a critical factor. A largescale<br />
SCE-based computer with a single, central processing volume and cylindrically symmetric temperature<br />
gradient was analyzed under the HTMT program 5 . The heat load at 4 K arises from both the SCE circuits and the<br />
cabling to and from room temperature. The cable heat load (estimated to be kWs) was the larger component, due to<br />
the large volume of data flow to the warm memory. Circuit heat load may be as small as several hundred watts. If all<br />
this heat at 4 K extracted via LHe immersion, a heat load of 1 kW would require a 1,400 liter/hour gas throughput rate.<br />
Several implementation approaches that would divide the total system into smaller, separately cooled modules will<br />
be discussed in the issues section. Both an approach with a few (but still large) modules and an approach with<br />
many smaller modules have potential virtues when it comes to the ease of wiring and minimization of cable loads.<br />
However, there are availability differences between large scale and small scale cryo-coolers. Therefore, the status<br />
will be presented for both types separately 6 .<br />
5 HTMT Program Phase IIII Final Report, 2002<br />
6 “Integration of Cryogenic Cooling with <strong>Superconducting</strong> Computers”, M. Green , Report for NSA panel.<br />
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