The integration limits y i measured from the NA are given as: y_{i} = frac{{varepsilon_{i} }}{{varepsilon_{text{L}} }}y_{text{L}}, (5 where ( varepsilon_{text{L}} ) and y L are the limiting strain (or the known strain) and its location, respectively; the latter is measured from the NA.
The joint frailty model for a recurrent event and a terminal event is defined as follows [ 5]: for subject i (i=1,…, N), let X ij be the j t h recurrent time (j=1,…, n i ) measured from the study origin (calendar time), D i be the death time and C i be the independent censoring time.
To illustrate this phenomenon, Figure 4 shows the average of σ i (f) measured from synthetic signals of known σ i (f).
K i was measured from Patlak plots of dynamic FDG-PET data [15, 16, 24].
I was measured from contact measurement of phantoms whereas I0 was measured from a Spectralon® target at a distance of 1 cm.
Heat capacities of sulfate, perrhenate, chloride, and iodide sodalites with the ideal formula Na8Al6Si6O24X2 (X = SO4, ReO4, Cl, I) were measured from 2 K to 300 K using a Quantum Design Physical Property Measurement System (PPMS).
The shifts ∆ν of amide I band (measured from 1,626 to 1,639 cm−l for SPhMDPOBn in pristine state) of 33 and 35 cm−l which occurred when SPhMDPOBn was immobilized on the silica surface may be caused by a weakening of the intramolecular hydrogen bonding of the SPhMDPOBn because the interaction with the silica surface as hydrogen bond with silanol groups is weaker than that in associates.
The shifts ∆ν of the amide I band (measured from 1,626 to 1,639 cm−l for SPhMDPOBn in the pristine state) of 33 and 35 cm−l which occurred when SPhMDPOBn was immobilized on the silica surface may be caused by a weakening of the intramolecular hydrogen bonding of the SPhMDPOBn because the interaction with the silica surface as hydrogen bond with silanol groups is weaker than that in the associates.
Thirdly, K i was directly measured from Dixon plot as an intercept on x-axis.
At this distance the diameter of each LED was 4.9 arc', center-to-center spacing was 7.4 arc', and the dimensions of the full array, i.e., measured from center-to-center of the outside elements, was 7.7 × 7.7 arc°.
The measured current in the photodiode, I m, is: Figure 5 Dark I-V characteristic measured from the fabricated radial p-Cu 2 O/n-TiO 2 nanowires.
