Exact(4)
for oscillation in a 3n dimensional potential well determined by the 3n × 3n matrix B. The 3n eigenvalues (Ω1)2,..., (Ω3n 2 of matrix B are squared frequencies of 3n independent one-dimensional oscillations along its eigenvectors.
In general, the Gini coefficient equals the sum of the squared frequencies or probabilities of a distribution and captures the concentration of a distribution (Gini 1921).
Using a perturbation approach, it is found that for a shear building, a reduction in instantaneous stiffness due to a yielding occurring in the bottom story will cause a greater absolute percentage change in eigenvalues (squared frequencies) of a lower mode than that of a higher mode.
The formula of δ, presented by Hankins, reads: (1) in which k is the number of items, m is the number of response options per item, n is the sample size and is the sum of squared frequencies of each score i.
Similar(56)
However, there is also a more subtle anomaly at ≈45 K were the gradient of the squared frequency changes.
Mean match probability was calculated as the sum of the squared genotype frequencies per locus.
The random match probability was calculated as the sum of squared haplotype frequencies based on mtDNA control region sequences.
Haplotype diversity (HD) was calculated analogous to GD. Match probability (MP) was calculated as the sum of squared haplotype frequencies.
Within our Ghana sample set the random match probability was calculated as the sum of squared CR frequencies, disregarding length variants at positions 16193, 309 and 573.
H values (expected heterozygosities for populations and combined populations) were calculated as 1 minus the sum of the squared allele frequencies at a locus.
The product of these two characteristic frequencies is equal to the squared resonant frequency of the layered system, times a dimensionless proportionality constant of the order 1.
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