Referring to the realization of deterministic matrix F on each CR user, frequency-selective surfaces (FSSs) [38] and random filtering [39, 40] can be utilized as effective approaches.
A contour is defined by non-zero grey level values aside the center circle, at a maximum distance r f on each side of the center circle.
The hypothesis that the observed JFF values are due almost exclusively to through-space Fermi-contact coupling together with the rapid rotation of TMF CF3 groups led to the conclusion that the "instantaneous" coupling constants for a specific pair of F atoms, one on each of the two neighboring CF3 groups in question, are nine times larger than the 8 20 Hz time-averaged values.
Figures 3, 4, 5, and 6 give the sensitivity, PPV, ACC, and F of each method on the testing dataset.
It is established by means of the quadratic interpolation approximation using three points (tj−2,f(tj−2)),ftj−1,f(tj−1)) and (tj,f(tj)) for the integrand f(t) on each small interval [tj−1,tj] (j⩾2), while the linear interpolation approximation is applied on the first small interval [t0,t1].
Likewise, the thrust F xi on each newly designed disc cutter is given by: F_{xi} = q_{xi} A_{x} = 2kleft( {1 + frac{uppi}{2} - alpha_{i} } right)A_{x}.
According to the theory presented in Ref. [22], the thrust F zi on each traditional disc cutter can be expressed as: F_{zi} = q_{zi} A_{z} = 2kleft( {1 + frac{uppi}{2}} right)A_{z}.
In fact, if f is a continuous function, then we can take a sequence of functions (mathrm{f}_{l}=mathrm{f}_{l} t,mathrm{x},mathrm{y})) that are T-periodic in the t-variable and locally Lipschitzian in the (x,y -variable,y -variablehrm{f}_{l}(t,mathrm{x},mathrm{y})}) converging to f uniformly on each compact subset of ([0,T]times mathbb{R}^{3}timesmathbb{R}^{3}).
Wilcoxon signed rank test was used for comparison of difference between pre- and post-treatment PPTs in medial knee (including 6 sites; A-F) and on each site.
