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By American Institute of Physics, Dwight E. Gray

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Eq. (2a-20)] is called the angular momentum of the rigid body about the origin. By expansion of the summand in Eq. (2a-21) after employing Eq. Ig• + "'gIg. 1•• + ""I•• ) where 1••, I •• , I .. " We have L. = "Zm,(y;' + z,') etc. (2a-35) I •• = "Zm;x;y. etc. By proper choice of axes (called "principal" axes) the products of inertia can be made to vanish. If we write (2a-36) I •• = MR' R' _ "Zm;(Yi' + z;') (2a-37) where M and M is the total mass of the rigid body, R is termed the "radius of gyration" about the x axis.

1 to 6 are not closed-ended. Other units compatible with the S1 can and will be added on the basis of: 1. Actions taken by subsequent General Conferences 2. Clear indication of need in specialized fields, following approval of the NBS Editorial Review Boards and the NBS Units and Usage Committee Artificial creations such as kilo angstrom and cubic angstrom are, for the most part, unnecessary and do more harm than good. They should be replaced by SI units as rapidly as possible. , electron-volt, are both meaningful and convenient.

Other units compatible with the S1 can and will be added on the basis of: 1. Actions taken by subsequent General Conferences 2. Clear indication of need in specialized fields, following approval of the NBS Editorial Review Boards and the NBS Units and Usage Committee Artificial creations such as kilo angstrom and cubic angstrom are, for the most part, unnecessary and do more harm than good. They should be replaced by SI units as rapidly as possible. , electron-volt, are both meaningful and convenient.

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