The National Ignition Facility has been used to compress deuterium - tritium to an average
areal density of ~ 1.0 ± 0.1 g cm -LRB--2), which is 67 % of the ignition requirement.
The figure shows an image of Mercury's surface (left; obtained using publicly available mosaic of Mercury from the MESSENGER spacecraft found at http://messenger.jhuapl.edu/) and a color - coded view of the global crater
areal density (right), obtained by measuring craters greater than 25 km.
Measurement of
areal density in the ablators of inertial - confinement - fusion capsules via detection of ablator (n, n «gamma) gamma - ray emission
Improved Performance of High
Areal Density Indirect Drive Implosions at the National Ignition Facility using a Four - Shock Adiabat Shaped Drive
Not exact matches
Assembly of High -
Areal -
Density Deuterium - Tritium Fuel from Indirectly Driven Cryogenic Implosions
They report that the silicon / graphite composite is mass - producible and it has superior battery performances with industrial electrode
density, high
areal capacity, and low amounts of binder.
Assembly of high -
areal -
density deuterium - tritium fuel from indirectly driven cryogenic implosions.
From what I inferred from the abstract, they say that the
areal power
density entering the ocean between 1955 and 2010 averaged 0.39 W / m ^ 2.
I haven't read the Levitis paper either but from the abstract it says that the
areal power
density entering the ocean between 1955 and 2010 averaged 0.39 W / m ^ 2.
The
areal difference between the mesopause and «surface» is 3.1 percent, due to the atmospheric transparency and
density gradient, the effective «day» of the middle atmosphere is 1 to 2 hours longer than a «surface» day.
The scheme depends on two parameters: the
areal fraction of the vertically - mixed region within the horizontal grid cell, and the
density difference between the mean and the unstratified profiles at the surface.