• Page 30, line 16. (C. A. Vanelli, 10/4/96) The expression for ω in equation (2.18) is singular when θ is π. To fix this, use the diagonal terms to determine the axis of rotation. • Page 40, figure 2.5. (W. Wray, 1/12/95) The expression p(t should be p(t) in the figure (occurs twice). • Page 75, line -2. (W. Wray, 1/12/95) SO(3) should be SO(2). • Page 114, line -6. (R. Mason, 4/16/95) The phr...

A chute was designed following the principles of Theory Sampling to minimize variations in powder flow and provide all particles flowing blends with same opportunity being selected as a sample. The design also reduces thickness allow analysis higher portion by near infrared spectrometer. that flowed through had Carr’s index values fluctuated between 23 25 percent, indicating passable flowabilit...

A prediction problem of the following variety is considered. A stationary random process w(.) of known spectrum is observed over 1 1 < a . Using these observed values, w(b) is to be predicted for some b with lbl>a. We present a physical interpretation of a solution to this problem due to Krein, which used the theory of inverse Sturm-Liouville problems. Our physical model involves a nonuniform l...

We introduce a Wilson line distribution function W τ (v) to study gluon saturation at small Feynman x F , or large τ = ln(1/x F ). This new distribution can be obtained from the distribution Wτ (α) of the Color Glass Condensate model and the JIMWLK renormalization group equation. W τ (v) is physically more relevant, and mathematically simpler to deal with because of unitarity of the Wilson line...

We introduce a Wilson line distribution function W τ (v) to study gluon saturation at small Feynman x F , or large τ = ln(1/x F ). This new distribution can be obtained from the distribution Wτ (α) of the Color Glass Condensate model and the JIMWLK renormalization group equation. W τ (v) is physically more relevant, and mathematically simpler to deal with because of unitarity of the Wilson line...