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The estimation of the speed of convergence comes from the Banach contraction principle.
To do this, an estimation of the speed of both the wheels must be performed using specific sensors.
In this paper, the kinematic model is refined with the estimation of the speed and the object size through the fractional transform along the distorted direction.
In relation to this, Clark, Perrone [16] have demonstrated that the estimation of the speed of large moving objects such as and specifically trains is likely to be erroneous.
In particular, conditions ensuring the existence of a periodic family of probability measures to which the law of v converges as time grows have been identified, together with a sharp estimation of the speed of mixing.
The statistical knowledge was then introduced into the model by performing a sequential learning of these parameters and an estimation of the speed field of the fluid flow starting from measurements.
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In the particular case when (c:= sup_{iin I}operatorname{Lip}(f_{i})<1), we have the following estimations of the speed of convergence (h(F_{mathcal{S}}^{[n]}(Y ,A leqfrac{c^{n}}{1-c}h(F_{mathcal{S}}(Y),Y)) for every (Yin B X)) and (d(A_{alpha})leq c^{n}d(A)) for every (alphainLambda_{n}).
In the particular case when (c:=sup_{iin I} operatorname{Lip}(f_{i})<1), we have the following estimations of the speed of convergence: d_{infty}bigl(H_{mathcal{S}}^{[n]}(f),pi_{0}bigr) leqfrac{c^{n}}{1-c}d_{infty}bigl(H_{mathcal{S}}(f),fbigr).
It is combined to a wind speed estimator that provides an estimation of the wind speed and the aerodynamic torque involved in the controller.
The ion data are used to assist the scientific interpretation of the energy spectra including (1) conversion of the temporal scales into the spatial scales using Taylor's frozen-in hypothesis and (2) estimation of the Alfvén speed (V A ), sound speed (c s ), and the gyrofrequency (Ω i ) and gyroradius (ρ i ) for thermal ions.
Based on our estimation of the ejection speed in the previous section, the ejection speeds were approximately v e = 145 and 185 m/s with drag coefficients of C D = 0.62 and 1.01, respectively.
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