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Prospero 8/4/2008 | 0 (0) | 41 | 0 | 0 | English
Williams, Boggs & Ratcliff, NASA JPL, California
Institute of Technology, Pasadena; Variations in rotation and orientation of the Moon are sensitive to solid-body tidal dissipation, dissipation due to relative motion at the fluid-core/solid-mantle boundary, and tidal Love number k2. more>>
BStennes 8/18/2008 | 0 (0) | 73 | 0 | 0 | English
Making decisions is critical to the success of an organization, but it is not always easy. This essay offers tips for overcoming procrastination and institutional inertia, so that you can become a more dynamic leader. more>>
Prospero 8/12/2008 | 0 (0) | 35 | 0 | 0 | English
Williams, Boggs & Ratcliff, JPL, Pasadena
Variations in rotation and orientation of the Moon are sensitive to solid-body tidal dissipation, dissipation due to relative motion at the fluid-core/solid-mantle boundary, and tidal Love number k2. There is weaker sensitivity to flattening of the core-mantle boundary (CMB) and fluid core moment of ... more>>
Prospero 7/29/2008 | 0 (0) | 52 | 0 | 0 | English
J. G. Williams, D. H. Boggs, J. T. Ratcliff and J. O. Dickey, Jet Propulsion Laboratory; Variations in rotation and orientation of the Moon are sensitive to solid-body tidal dissipation, dissipation due to relative motion at the fluidcore/solid-mantle boundary, and tidal Love number k2. There is weaker sensitivity to flattening of the core-mantle ... more>>
Prospero 8/5/2008 | 0 (0) | 33 | 0 | 0 | English
Opanasenko & Shkuratov, Astronomical Institute of Kharkov National University, Kharkov, Ukraine; Swirls are albedo structures, occurring
on the Moon and Mercury, which are considered
to be results of cometary or meteoroid swarm encounters. The Reiner Gamma Formation (RGF) is the best swirl example on the Moon located in the western portion of the ... more>>
hmharky 4/23/2008 | 0 (0) | 67 | 4 | 0 | English
LisaB1982 5/31/2008 | 0 (0) | 26 | 2 | 0 | English
ProfessionalDocument 7/29/2008 | 0 (0) | 12 | 0 | 0 | English
jackl17 10/30/2008 | 0 (0) | 0 | 0 | 0 | English
shwarma 11/3/2008 | 0 (0) | 1 | 0 | 0 | English
xarrnet 10/31/2008 | 0 (0) | 1 | 0 | 0 | English
ProfessionalDocument 7/29/2008 | 0 (0) | 12 | 0 | 0 | English
Moment of Inertia, and Stress Area. 431 To find the Moment of Inertia of any Beam Section. -Proceed as in the last construction and find Z. nd I = Zjy.* So for rectangular sections bJP h ^bh* 62 12
Then Z = y . \ X — ---
Stress areas for circle, hollow circle, triangle, and hollow •ectangle we shewn in Fig. 385, being measured as in Fig. 372 mean ... more>>
LisaB1982 4/22/2008 | 0 (0) | 99 | 3 | 0 | English
hmharky 4/23/2008 | 0 (0) | 28 | 0 | 0 | English
LisaB1982 5/31/2008 | 0 (0) | 40 | 0 | 0 | English
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