Impact of the Order Parameter

Expressions (46) and (53) allow us also to analyse the impact of the LCAO parameter c on the first-order and second-order polarizabilities, a and /3. We assume that the excitation energy does not vary with c as discussed above and... 

The overall impact of the various parameters was found to be in the following order shear rate > mixing time > temperature. The combination of slower shear, shorter mixing time, and lower reaction temperature consistently produced quality amorphous MBP. A similar observation was made in the experiment with continuous mode procedure. 

One further question that has a substantial impact on the application of modeling techniques to biomedical problems is the choice of the design. Suppose that in our Gompertz tumor growth example we wanted to decide, given the results of some pilot experiments, when it is most useful to observe the tumor volume. In other words, we wish to choose the time points at which we obtain tumor volume observations in order to maximize the precision of the resulting parameter estimates. 

From this equation we can see that, in the problem considered, the characteristic size (in atomic units) is of the order of yfz consequently, the time of collision has the order of y/z/v, where v is the relative velocity of the colliding particles. The probability of charge transfer during the collision with the impact parameter p can be estimated if we multiply the probability of tunneling per unit time by the time of collision... 

In summary, in order to minimize the impact of the lost crude cost on the total cost, the operating parameters are adjusted to improve the yield. 

The impact parameter can be estimated simply from the following consideration the transverse electrostatic pulse contains frequencies of the order of v/b, where v is the velocity of the fast electron. Thus a core electron bound with an energy AE can only be promoted to empty states above the Fermi level in the conduction band if rfundamental property of the radiation can also be seen by explicitly integrating the resultant electric field at an atomic site a distance b away (as given in eq. (3.12)), over the momentum space d q giving ... 

More precisely, we first pay attention to intrinsic conductivity. Indeed, its measurement is very difficult, so the values commonly used vary in a large range, covering several orders of magnitude. Concerning the gas, we study the impact of the conductivity value which is much more difficult to evaluate than the liquid one. Particularly, we wonder if this parameter can induce a heat-pipe effect. We also determine the influence of gas boundary condition. An hypothesis consists in considering the gas confined in the repository chamber, another one permits it to escape. Finally, we tried to evaluate the influence of mechanical boundary condition, which depends on the width of void between the EB and the canister. 

The morphology of the resulting solid material depends both on the material structure (crystalline or amorphous, composite or pure, etc.) and on the RESS parameters (temperature, pressure drop, distance of impact of the jet against the surface, dimensions of the atomization vessel, nozzle geometry, etc.)[ l It is to be noticed that the initial investigations consisted of pure substrate atomization in order to obtain very line particles (typically of 0.5-20 m diameter) with narrow diameter distribution however, the most recent publications are related to mixture processing in order to obtain microcapsules or microspheres of an active ingredient inside a carrier. 

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