Inertial confinement fusion : ICF annual report by Lawrence Livermore National Laboratory
By Lawrence Livermore National Laboratory
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This station includes a “set up” microscope for manipulation and overview of the foams, a calibrated characterization microscope for checking the dimensional tolerances, a precision balance for confirming the weight of each foam and a computer with CD–ROM writing ability. All data is directly entered into the computer and a CD–ROM is created for each order. As we improved the speed with which we could produce foams, we gave ourselves time to address quality issues. The two primary concerns that SNL voiced was the need for tighter dimensional tolerances and low foam densities.
Hoppe (GA). 2. SPECTROSCOPIC THICKNESS DETERMINATION OF SHELL LAYERS Reflection spectra of thin films (from <1 to >50 µm thick) show intensity oscillations (Fig. 2–13) which allow one to accurately calculate their thickness. The oscillations come from interference between the film’s front and back surface reflections. The path difference between the two beams is twice the optical thickness of the film (optical thickness = physical thickness × index of refraction). Even (odd) multiples of one-half give minima (maxima) in the reflected intensity.
Pinholes may have resulted when large nodules were knocked off the surface when shells collided against each other during bounce coating. The presence of numerous grain boundaries and pinholes in the coatings on shells makes the observed relatively fast permeation rates for argon and D2 somewhat understandable. 2 µm SiO2 on 900 × 10 µm GDP Shell Fig. 2–9. 2 µm glass coating on a ~900 diameter × 10 µm GDP shell. The coating had developed numerous microcracks when examined after coating. 4 µm or thicker.