Exact(6)
This solution is valid for the equivalent heat transfer problem also.
This solution is valid provided that there is no change in the active constraints of the system.
This solution is valid for any non-uniform far load and is finite and exact in the case of polynomial far field.
This approach is based on theoretical results obtained in former works and furnishes not only a local solution to the problem but also an estimate for the state space region where this solution is valid.
The following argument shows that this solution is valid for 91≤r≤95.
It is a feasibility study but the first results prove that this solution is valid if we consider the needed ressources.
Similar(53)
That this solution was valid was confirmed by the observation of several residue substitutions in the electron density map, convergence of the CNS refinement minimizations steps using non-crystallographic restraints at 1.6 Å resolution, and improved iterative automatic reconstruction of this model using the ARP/wARP procedure [25].
end{cases} In this case, the solution is valid for all (xinmathbb{R}).
In both the dc polarography and in the square wave polarography, the Stokes Einstein Ilkovič equation connecting polarographic current and viscosity of the solution, is valid only in the case of monomeric solutions.
The solution is valid only after this time.
Although the well-known harmonic vibration solution is valid only when the reciprocating motion is slow, this approximate solution is valid for a wide range of both motions, reciprocating and vibrating.
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