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The capacity decays from the initial value of 922 to 710 mAh g−1 in the second cycle.
For (textbf{v}invarGamma_), the value function is calculated assuming that the control is turned off for an interval ([0, hat{t}]), during which the system decays from the initial condition (textbf{v}(0)=[v_{1} v_{2}]^{T}) to a point (textbf{v}( hat{t}) = [hat{v}_{1} hat{v}_{2}]^{T}) on the curve Γ.
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Kinitial was taken as the steepest rate of decay from the initial collection time points.
Remarkably, at the end of floating, the specific capacitance calculated at 5 A g−1 was 120 F g−1 (∼25% decay in capacitance from the initial value 160.5 F g−1 at 5 A g−1) suggesting good stability of the device over a long period of time (∼8 days).
After reassessing all the brains from patients diagnosed with dementia, including those with large areas of vascular decay that were excluded from the initial study, they claimed that senile plaques accounted for dementia in over 50% of cases, with only 17% being due to arteriosclerosis alone and 18% showing a mixed picture (Tomlinson, Blessed and Roth, 1970).
To follow the estimation method of Segel and Slemrod [ 1], we consider the case when R decays from its initial condition.
The radiochemical yield of [18F]CFT from the initial [18F]F-, decorrectedctod thethendnd of bombardment, was 3.2 ± 1.0%.
Finally, it is demonstrated that the usual sound power estimate based on measurement of the spatial average of the mean square pressure is unbiased, provided that the losses of the room are deduced from the initial rates of decay.
The equivalent sound absorption area in a rectangular reverberant room can be derived from the initial first and second derivatives (initial decay rate of the time derivative) of the ensemble and space-averaged sound energy decay curve.
Radiochemical yields [RCY] were calculated from the initial amount of [18F]F- and decay corrected to the end of bombardment [EOB].
In such a decay the initial kinetic energy is zero.
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