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NASA Scientific and Technical Aerospace Reports

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20040068248 Lawrence Livermore National Lab., Livermore, CA<br />

Acoustically-Driven Microfluidic Systems<br />

Wang, A. W.; Benett, E. J.; Tarte, L. R.; Jun. 23, 2000; 10 pp.; In English<br />

Report No.(s): DE2004-15006374; UCRL-JC-138305; No Copyright; Avail: Department of Energy Information Bridge<br />

We have demonstrated a non-contact method of concentrating <strong>and</strong> mixing particles in a plastic microfluidic chamber<br />

employing acoustic radiation pressure. A flaw cell package has also been designed that integrates liquid sample interconnects,<br />

electrical contacts <strong>and</strong> a removable sample chamber. Experiments were performed on 1, 3, 6, <strong>and</strong> 10(micro)m polystyrene<br />

beads. Increased antibody binding to a solid-phase substrate was observed in the presence of acoustic mixing due to improve<br />

mass transport.<br />

NTIS<br />

Acoustic Emission; Sound Waves; Mass Transfer<br />

20040068252 Lockheed Martin Corp., Syracuse, NY, USA<br />

Methods of Measuring Lock-In Strength <strong>and</strong> their Application to the Case of Flow over a Cavity Locking into a Single<br />

Side Branch Resonator<br />

Mendelson, R. S.; Apr. 2003; In English<br />

Report No.(s): DE2004-821511; LM-03K030; No Copyright; Avail: National <strong>Technical</strong> Information Service (NTIS)<br />

Lock-in is a non-linear interaction between a flow induced noise source <strong>and</strong> a resonator when their respective frequencies<br />

are near each other. Lock-in has been reported under many different labels <strong>and</strong> for many different applications. There is a need<br />

however for a consistent community wide method to measure the strength of lock-in so that data from different tests <strong>and</strong><br />

different source/resonator combinations can be compared. This paper discusses three methods for measuring lock-in strength.<br />

The first, Resonant Response Method, (RRM) subtracts (in the decibel scale) the linear modal response of the resonator to<br />

broadb<strong>and</strong> (BB) flow noise from the resonant response when lock-in occurs. The second, Quality Factor Method (QFM) tracks<br />

the change in quality factor of the resonant response. The third defines the strength in terms of the difference between peak<br />

response <strong>and</strong> the local BB levels.<br />

NTIS<br />

Acoustics; Resonators<br />

20040068370 Sverdrup Technology, Inc., Huntsville, AL, USA, <strong>NASA</strong> Marshall Space Flight Center, Huntsville, AL, USA<br />

Measuring Thermal Conductivity at LH2 Temperatures<br />

Selvidge, Shawn; Watwood, Michael C.; [2004]; 1 pp.; In English; 45th AIAA/ASME/ASCE/AHS/ASC Structures,<br />

Structural Dynamics <strong>and</strong> Materials Conference, 19-22 Apr. 2004, Palm Springs, CA, USA<br />

Contract(s)/Grant(s): NAS8-00187; No Copyright; Avail: Other Sources; Abstract Only<br />

For many years, the National Institute of St<strong>and</strong>ards <strong>and</strong> Technology (NIST) produced reference materials for materials<br />

testing. One such reference material was intended for use with a guarded hot plate apparatus designed to meet the requirements<br />

of ASTM C177-97, &quot;St<strong>and</strong>ard Test Method for Steady-State Heat Flux Measurements <strong>and</strong> Thermal Transmission<br />

Properties by Means of the Guarded-Hot-Plate Apparatus.&quot; This apparatus can be used to test materials in various<br />

gaseous environments from atmospheric pressure to a vacuum. It allows the thermal transmission properties of insulating<br />

materials to be measured from just above ambient temperature down to temperatures below liquid hydrogen. However, NIST<br />

did not generate data below 77 K temperature for the reference material in question. This paper describes a test method used<br />

at <strong>NASA</strong>’s Marshall Space Flight Center (MSFC) to optimize thermal conductivity measurements during the development of<br />

thermal protection systems. The test method extends the usability range of this reference material by generating data at<br />

temperatures lower than 77 K. Information provided by this test is discussed, as are the capabilities of the MSFC Hydrogen<br />

Test Facility, where advanced methods for materials testing are routinely developed <strong>and</strong> optimized in support of aerospace<br />

applications.<br />

Author<br />

Liquid Hydrogen; Thermal Conductivity; Temperature Distribution; <strong>Aerospace</strong> Engineering<br />

20040070710 <strong>NASA</strong> Ames Research Center, Moffett Field, CA, USA<br />

Adaptive Low Dissipative High Order Filter Methods for Multiscale MHD Flows<br />

Yee, H. C.; Sjoegreen, Bjoern; January 13, 2004; 1 pp.; In English; No Copyright; Avail: Other Sources; Abstract Only<br />

Adaptive low-dissipative high order filter finite difference methods for long time wave propagation of shock/turbulence/<br />

combustion compressible viscous MHD flows has been constructed. Several variants of the filter approach that cater to<br />

88

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