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The BEC is described by the Gross Pitaevskii equation, which can be solved numerically using the Crank Nicholson method.
The theoretical model also introduces an equation which can be used to predict the optimum bed length.
Multiscale methods approximate it by another partial differential equation which can be numerically simulated in a reasonable time.
These assumptions lead to a saturation equation which can be solved by standard methods used for thermal problems.
Thus according to Bernoulli's equation, which can be relied on outside the boundary layer, the pressure near Q is less than it is near P and P′.
The above phenomena could be illustrated in the frame of approximately continuous phase transition derived Belov Goryaga equation, which can be modified for ferroelectrics.
A universal equation which can be used to predict the fluence required of any bacteria with a shoulder: H = (0.914 ± 0.055) * (BSI E * (Log I) + H0.
The dynamics at each node of the coupled map lattices is described by a general difference equation, which can be of chaotic or others.
The starting point was the integral equation which can be considered as the general mathematical model of a hydrodynamically linear chemical apparatus.
The total effect of all these causes can be described by a simple equation which can be derived from the rigorous mathematical solution by introducing reasonable simplifying assumptions.
We present an accurate and efficient algorithm for the solution of the retarded time equation, which can be used both in subsonic and supersonic flow regimes.
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