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CEC Abstracts in PDF format (as of 7/3/07) - CEC-ICMC 2013

CEC Abstracts in PDF format (as of 7/3/07) - CEC-ICMC 2013

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<strong>CEC</strong> 20<strong>07</strong> - <strong>Abstracts</strong><br />

C3-K Thermal Insulation Systems - II<br />

C3-K-01 Vacuum-Insulated, Flexible Cryostats for Long<br />

HTS Cables: Requirements, Status and Prospects<br />

M.J. Gouge, J.A. Demko, ORNL; J.F. Maguire,<br />

AMSC; M.L. Roden, Southwire Company; C.S. Weber,<br />

SuperPower, Inc..<br />

Several high temperature superconduct<strong>in</strong>g (HTS) cable demonstration<br />

projects have begun operation on the electric grid <strong>in</strong> the l<strong>as</strong>t year with<br />

the liquid nitrogen-cooled cable conta<strong>in</strong>ed <strong>in</strong> one or more vacuum<strong>in</strong>sulated,<br />

flexible cryostats with lengths up to 600 meters. These grid<br />

demonstration projects are prototypes <strong>of</strong> the anticipated commercial<br />

market which will require superconduct<strong>in</strong>g cable lengths <strong>in</strong> the<br />

multiple kilometer range with the vacuum-jacketed cryostats <strong>in</strong><br />

underground ducts provid<strong>in</strong>g acceptable thermal <strong>in</strong>sulation for<br />

decades. The current state-<strong>of</strong>-the art for flexible cryostats (<strong>in</strong>stallation<br />

constra<strong>in</strong>ts, heat loads with a good and degraded vacuum, impact <strong>of</strong><br />

cable bends, getter lifetime and reliability) is discussed. Further<br />

development needed to meet the challeng<strong>in</strong>g commercial HTS cable<br />

application is outl<strong>in</strong>ed.<br />

Research sponsored by the U.S. Department <strong>of</strong> Energy - Office <strong>of</strong><br />

Electricity Delivery and Energy Reliability, Superconductivity<br />

Program for Electric Power Systems under contract DE-AC05-<br />

00OR22725 with Oak Ridge National Laboratory, managed and<br />

operated by UT-Battelle, LLC.<br />

C3-K-02 Heat Flow Me<strong>as</strong>urement and Analysis <strong>of</strong><br />

Thermal Vacuum Insulation<br />

C. Laa, C. Hirschl, J. Stipsitz, Austrian Aerospace<br />

GmbH.<br />

A new k<strong>in</strong>d <strong>of</strong> calorimeter h<strong>as</strong> been developed to obta<strong>in</strong> specific<br />

material parameters needed for the analysis <strong>of</strong> thermal vacuum<br />

<strong>in</strong>sulation. A detailed description <strong>of</strong> the me<strong>as</strong>ur<strong>in</strong>g device and the<br />

me<strong>as</strong>urement results will be given <strong>in</strong> this paper.<br />

This calorimeter facility allows to me<strong>as</strong>ure the heat flow through the<br />

<strong>in</strong>sulation under vacuum conditions <strong>in</strong> a wide temperature range from<br />

liquid nitrogen to ambient. Both boundary temperatures can be chosen<br />

with<strong>in</strong> this range. The <strong>in</strong>sulation can be characterized at high vacuum<br />

or under degraded vacuum, the latter us<strong>in</strong>g helium or nitrogen g<strong>as</strong>.<br />

The mechanisms <strong>of</strong> heat transfer have been <strong>in</strong>vestigated, namely<br />

<strong>in</strong>frared radiation between the reflective layers <strong>of</strong> the <strong>in</strong>sulation and<br />

conduction through the <strong>in</strong>terleav<strong>in</strong>g spacer material. A mathematical<br />

description <strong>of</strong> the heat flow through the <strong>in</strong>sulation h<strong>as</strong> been derived.<br />

B<strong>as</strong>ed on this the heat flow for a typical <strong>in</strong>sulation material h<strong>as</strong> been<br />

calculated by f<strong>in</strong>ite element analysis by use <strong>of</strong> the s<strong>of</strong>tware tool<br />

ANSYS. Such a transient calculation is needed to determ<strong>in</strong>e the time<br />

to reach thermal equilibrium, which is mandatory for a proper<br />

<strong>in</strong>terpretation and evaluation <strong>of</strong> the me<strong>as</strong>urement.<br />

The new <strong>in</strong>sulation me<strong>as</strong>urement results comb<strong>in</strong>ed with the proposed<br />

type <strong>of</strong> analysis can be applied to better understand the thermal<br />

behavior <strong>of</strong> any k<strong>in</strong>d <strong>of</strong> cryogenic system.<br />

C3-K-03 Robust Multilayer Insulation for Cryogenic<br />

Systems<br />

J.E. Fesmire, B.E. Scholtens, NASA KSC; S.D.<br />

Augustynowicz, Sierra Lobo, Inc..<br />

New requirements for thermal <strong>in</strong>sulation <strong>in</strong>clude robust multilayer<br />

<strong>in</strong>sulation (MLI) systems that work for a range <strong>of</strong> environments from<br />

high vacuum to no vacuum. Improved MLI systems must be simple<br />

to <strong>in</strong>stall and ma<strong>in</strong>ta<strong>in</strong> while meet<strong>in</strong>g the life-cycle cost and thermal<br />

performance objectives. Performance <strong>of</strong> MLI systems <strong>in</strong> actual use<br />

h<strong>as</strong> been shown to be much worse than the ideal c<strong>as</strong>e. Industry<br />

products us<strong>in</strong>g robust MLI can benefit from improved cost-efficiency<br />

and system safety. Spacecraft that must store cryogens dur<strong>in</strong>g all<br />

mission ph<strong>as</strong>es, <strong>in</strong>clud<strong>in</strong>g orbital/lunar service (high vacuum) and<br />

ground launch operations (no vacuum) are planned. Future cryogenic<br />

spacecraft for the s<strong>of</strong>t vacuum environment <strong>of</strong> Mars are also<br />

envisioned. Novel materials have been developed to operate <strong>as</strong><br />

excellent thermal <strong>in</strong>sulators at vacuum levels that are much less<br />

str<strong>in</strong>gent than the absolute high vacuum requirement <strong>of</strong> current MLI<br />

systems.<br />

One such robust system, Layered Composite Insulation (LCI), h<strong>as</strong><br />

been developed at the Cryogenics Test Laboratory <strong>of</strong> NASA Kennedy<br />

Space Center. The experimental test<strong>in</strong>g and development <strong>of</strong> LCI is<br />

the focus <strong>of</strong> this paper. Compared to MLI under cryogenic<br />

conditions, LCI thermal performance is shown to be six times better at<br />

s<strong>of</strong>t vacuum and similar at high vacuum. The apparent thermal<br />

conductivity (k-value) and heat flux data for LCI systems are<br />

compared with other MLI systems.<br />

C3-K-04 Synthesis on the multilayer cryogenic vacuum<br />

<strong>in</strong>sulation modell<strong>in</strong>g and me<strong>as</strong>urements<br />

M. Chorowski, J. Pol<strong>in</strong>ski, Wroclaw University <strong>of</strong><br />

Technology.<br />

A thermodynamic approach towards <strong>in</strong>sulation systems <strong>in</strong> cryogenic<br />

eng<strong>in</strong>eer<strong>in</strong>g is proposed. A mathematical model <strong>of</strong> the heat transfer<br />

through multilayer <strong>in</strong>sulation (MLI) h<strong>as</strong> been developed and<br />

experimentally verified. The model comprises both physical and<br />

eng<strong>in</strong>eer<strong>in</strong>g parameters determ<strong>in</strong><strong>in</strong>g the MLI performance and enables<br />

a complex optimisation <strong>of</strong> the <strong>in</strong>sulation system <strong>in</strong>clud<strong>in</strong>g the choice<br />

<strong>of</strong> the <strong>in</strong>sulation location <strong>in</strong> a vacuum space. The model takes <strong>in</strong>to<br />

account an <strong>in</strong>terstitial (<strong>in</strong>terlayer) g<strong>as</strong> pressure and a shield – spacer<br />

thermal contact resistance variation with the MLI layer density. The<br />

paper presents the discussion <strong>of</strong> MLI performance <strong>in</strong> different<br />

conditions and provides comparison <strong>of</strong> computation results with<br />

experimental reference data. The optimisation <strong>of</strong> the <strong>in</strong>sulation for<br />

different boundary conditions is analysed and concluded.<br />

C3-K-05 Thermal Performance Comparison <strong>of</strong> Gl<strong>as</strong>s<br />

Microsphere and Perlite Insulation Systems for Liquid<br />

Hydrogen Storage Tanks<br />

J.P. S<strong>as</strong>s, J.E. Fesmire, D.L. Morris, NASA KSC; Z.F.<br />

Nagy, S.D. Augustynowicz, Sierra Lobo, Inc.; S.J.<br />

Sojourner, ASRC Aerospace.<br />

A technology demonstration test project w<strong>as</strong> conducted by the<br />

Cryogenics Test Laboratory at the Kennedy Space Center (KSC) to<br />

provide comparative thermal performance data for gl<strong>as</strong>s microsphere<br />

and perlite <strong>in</strong>sulation for liquid hydrogen tank applications. Two<br />

identical 1/15th scale versions <strong>of</strong> the 850,000 gallon spherical liquid<br />

hydrogen tanks at Launch Complex 39 at KSC were custom designed<br />

and built to serve <strong>as</strong> test articles for this test project. Evaporative<br />

(boil-<strong>of</strong>f) calorimeter test protocols, <strong>in</strong>clud<strong>in</strong>g liquid hydrogen and<br />

liquid nitrogen, were established to provide tank test conditions<br />

characteristic <strong>of</strong> the large storage tanks that support the Space Shuttle<br />

launch operations. This paper provides comparative thermal<br />

performance test results for gl<strong>as</strong>s microspheres and perlite for a wide<br />

range <strong>of</strong> conditions. Limited results for aerogel <strong>in</strong>sulation material<br />

are also <strong>in</strong>cluded. Aerogel-b<strong>as</strong>ed <strong>in</strong>sulation systems are targeted for<br />

non-evacuated liquid oxygen tank applications due to cost and<br />

performance parameters. Thermal performance <strong>as</strong> a function <strong>of</strong><br />

cryogenic commodity (hydrogen and nitrogen), vacuum pressure,<br />

<strong>in</strong>sulation fill level, tank liquid level, and thermal cycles will be<br />

presented.<br />

Fund<strong>in</strong>g w<strong>as</strong> provided by the NASA Space Operations Mission<br />

Directorate under the Internal Research and Development project<br />

New Materials and Technologies for Cost-Efficient Storage and<br />

Transfer <strong>of</strong> Cryogens.<br />

Page 43 <strong>of</strong> 53

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