respectively, (F(mu ^{prime }_{1})) is easily evaluated from Eq. (2), M=Q_{G}left[1-left(frac{1-2^{-1/alpha}}{1-ptimes2^{-1/alpha}}right)^{1/lambda}right] is the median of X, (mu ^{prime }_{1}=mathrm {E}(X)) comes from (18) and m 1 y) is the first incomplete moment of X determined from (22) with r=1.
Such an error is limited and can be easily evaluated for each obstacle with (17).
We derive quantities which are independent on the detailed mapping of the model fiber to the biological chromosome, but can be easily evaluated both from simulational data as well as from experimental data.
Clearly, c n,i can be easily evaluated numerically from c n,0,…,c n,i−1 and then from the quantities a 0,…,a i. Next, we derive an expansion for the argument of Q G in Eq. (5) A=1-frac{ 1-u^{1/A=1-frac{ 1-u^{dA=1-frac{ 1-u^{lpha})^{1/alpha}}}.
The integrand in (16) can be easily evaluated since the PDFs are known from (10).
The prognosis and clinical curative effects could be easily evaluated under that CIK cells were generated from universal sources.
By recording electrochemical responses from AgNPs, initial concentration of PSA can be easily evaluated.
Lastly, as digital templates are now readily available from manufacturers, design changes and newer prostheses can be easily evaluated and comparisons can be made to previously tested prostheses under identical experimental conditions.
Parameters p, x can be easily evaluated with small uncertainty during the measurement by exploitation of the scale factor from pixels to millimeters in the reference frame.
Yet if a city is to a great extent a cultural mirror, it cannot be easily evaluated simply by observing its effects.
