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Thermal Performance of Cryogenic Multilayer Insulation at Various Layer Spacings (Paperback)
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Thermal Performance of Cryogenic Multilayer Insulation at Various Layer Spacings (Paperback)
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Multilayer insulation (MLI) has been shown to be the best
performing cryogenic insulation system at high vacuum (less that 10
(exp 3) torr), and is widely used on spaceflight vehicles. Over the
past 50 years, many investigations into MLI have yielded a general
understanding of the many variables that are associated with MLI.
MLI has been shown to be a function of variables such as warm
boundary temperature, the number of reflector layers, and the
spacer material in between reflectors, the interstitial gas
pressure and the interstitial gas. Since the conduction between
reflectors increases with the thickness of the spacer material, yet
the radiation heat transfer is inversely proportional to the number
of layers, it stands to reason that the thermal performance of MLI
is a function of the number of layers per thickness, or layer
density. Empirical equations that were derived based on some of the
early tests showed that the conduction term was proportional to the
layer density to a power. This power depended on the material
combination and was determined by empirical test data. Many authors
have graphically shown such optimal layer density, but none have
provided any data at such low densities, or any method of
determining this density. Keller, Cunnington, and Glassford showed
MLI thermal performance as a function of layer density of high
layer densities, but they didn't show a minimal layer density or
any data below the supposed optimal layer density. However, it was
recently discovered that by manipulating the derived empirical
equations and taking a derivative with respect to layer density
yields a solution for on optimal layer density. Various
manufacturers have begun manufacturing MLI at densities below the
optimal density. They began this based on the theory that
increasing the distance between layers lowered the conductive heat
transfer and they had no limitations on volume. By modifying the
circumference of these blankets, the layer density can easily be
vari
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