A
standardized way of comparing the thermal performance of different
pipelines in different sizes is needed. Vendor
data for vacuum-insulated piping are typically given in heat leak rate
per unit length (watt per meter [W/m]) for a specific diameter pipeline.
An overall apparent thermal conductivity – k-value – for
actual field installations (koafi) is therefore proposed as a more generalized
measure for thermal performance comparison and design calculation. The
total system includes the inner piping, the insulation material layers,
the outer piping, and other items such as spacers and getters. The koafi provides a direct correspondence to the k-values reported for insulation
materials and illustrates the large difference between ideal multilayer
insulation (MLI) and actual MLI performance.
Ambient heat transfer into a cryogenic pipeline comes through several
paths including valves, connectors, instrumentation, and insulation.
A common
type of thermal insulation system is MLI. MLI systems come in many
varieties and must be tailored to the specific application. The
performance of MLI
is known to be sensitive to localized compression effects and trapped
residual gases produced by the combined mechanical influences
of bending and spacers.
Bending-type mechanical effects come from four sources: bending, as
in handling and installation; thermal contraction and expansion;
line pressure
reaction forces; and the weight of the line (sagging). Spacers are
employed in the design of vacuum-jacketed lines to keep the inner
line concentric
within the outer line during manufacturing and to counteract these
mechanical effects during operation. Spacers are made from low-thermal-conductivity
materials to minimize heat conduction.
In this experimental research study, a section of insulated piping
was tested under cryogenic vacuum conditions, including simulated
spacers and
bending. Several different insulation systems were tested using a
1-meter-long cylindrical cryostat test apparatus. The simulated
spacers tests showed
significant degradation in the thermal performance of a given insulation
system. The results of the simulated spacers test are given in figure
1. The spacer simulation shows a significant increase in the rate
of heat
transfer for the high-vacuum tests. For C123 in comparison to C124
the k-value increased from 0.09 to 0.15 milliwatt per meter-kelvin
(mW/m-K)
(a 67-percent increase in heat transfer).
Figure 2 provides a convenient design tool for estimating heat loads
(W/m) for different line sizes and different koafi. The experimental
laboratory
data can be compared with manufacturers’ typical data for
a 60- x 110-mm line: 2.30 W/m (flexible) and 0.75 W/m (rigid).
Converting these typical
heat leak values into their thermal conductivity equivalents, we
obtain koafi of 0.99 mW/m-K (flexible) and 0.32 mW/m-K (rigid).
The koafi method
is being used by the Cryogenics Test Laboratory to provide practical
engineering information for specific system designs and applications.
Contact: J.E. Fesmire (James.Fesmire-1@ksc.nasa.gov), YA-C2, (321)
867-7557
Participating Organization: Dynacs Inc. (Dr. S.D. Augustynowicz)
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Figure 1. Variation of Apparent Thermal Conductivity With Cold Vacuum
Pressure, Spacer Simulation Results
Figure 2. Variation of Heat Leak Rate With Diameter Ratio (Do/Di) for
koafi From 0.01 to 10 mW/m-K and Boundary Temperatures of 300 K and 77
K
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