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Both panning methods A and B were devised to perform optimal left to right balancing.
The trajectories of the actual ((nu_{text{s}} )) and estimated (left( {hat{nu }_{text{s}} } right)) slip velocities, as shown in Fig. 8, converge to some value near the optimal (left( {nu_{text{s}}^ right)) slip velocities.
Fluids were given to achieve an optimal left atrial pressure.
Optimal VV delay is less likely to significantly contribute to CRT response, especially in patients with optimal left ventricular lead positions.
Volume resuscitation (crystalloids, colloids and blood transfusions) was performed to achieve an optimal left arterial pressure, which was estimated by the pulmonary capillary wedge pressure reaching the plateau value for left ventricular stroke work.
Fluids were administered to achieve optimal left ventricular filling pressure, reaching the plateau value for left ventricular stroke work.
Similar(51)
Exercise effects on sleep in fit healthy people have been difficult to determine because their sleep is close to optimal, leaving little room for improvement.
In the other extreme, when growth durations are frequently shorter than a limit, a pessimistic strategy becomes optimal: leaving the protected state to resume growth when stress ceases can reduce the long term fitness.
Such evolutionary trends may lag behind what would be optimal, leaving opportunities for humans to accelerate adaptation.
Then, the resulting optimal point (left { {left { {mathbf {W}_{k0}^ right }_{k = 1}^{K},mathbf {V}_{0}^,mathbf {Sigma }_{0}^ right }) which leads to non-negative objective value of problem (45) can be selected as the feasible initial point.
Next, we proof the second part of Theorem 1. Suppose we achieved the optimal solution (left { {{{mathbf {W}}^{ast } }, {{mathbf {V}}^{ast } }, {mathbf {V}}_{0}^{ast }, {rho ^{ast }}, {t^{ast } }} right }) of (7), where the W ∗ is given in (9) and μ n >0, i.e., rank(W ∗)>1.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com