By Jim Goodall
F-117 Stealth in motion КНИГИ ;ВОЕННАЯ ИСТОРИЯ Издательство: Squadron/Signal publicationsСерия: plane quantity 115Автор(ы): Jim GoodallЯзык: EnglishГод издания: 1991Количество страниц: 52ISBN: 0-89747-259-4Формат: pdfРазмер: 13.0 mbRapid eighty five
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51, one obtains ln éë - ln (1 - Fm (d )) ùû = n ( ln(d ) - ln(d)). 52) Therefore, n is the slope of this line and δ can be obtained from the expression d= 16 dmM . 53) 1. 51: n -1 dFm (d ) n æ d ö = ç ÷ dè dø d (d ) f m (d ) = æ é æ d ön ù ö exp ç ê - ç ÷ ú ÷. 56) which leads to the relationship for the statistical parameters of this distribution ¥ òd 0 a æa ö f m (d )d (d ) = daG ç + 1 ÷. 5 Nukiyama–Tanasawa Distribution The Nukiyama–Tanasawa distribution is a more general distribution from which the Rosin–Rammler distribution is a special case.
The measure of the length in the first stage of the curve is N = 1. In the second stage, the length scale is Ls = 1/3 and the number of segments N = 4. In the third stage, the length scale is Ls = 1/9 and the number of segments N = 16. In terms of the original units, the total length of the curve is 4/3 units in the second stage, 16/9 in the third stage, and so on. For self-similar objects, such as this curve, there is a fundamental dimension, the fractal dimension, Lf, which does not change with the scale of measurement.
1 shows schematically the last three diameters or sizes for a particle that appears as an elongated parallelepiped. 1 A schematic diagram of the three equivalent diameters, dV, dA , and dL , for a particle with the shape of a parallelepiped. diameters, which are also depicted, vary significantly in magnitude. Because of the significant variability, a precise definition or measurement of the size of particles, bubbles, and drops must include how this size has been defined or measured (Michaelides, 2014).