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An example of a weak form of Eq. (2) satisfies (Formula presented) for any sufficiently smooth test function (Formula presented) where the integrals are over all time and space. This expression is obtained by multiplying Eq. (2) by (Formula presented) and integrating twice by parts with no-flow boundary conditions, (Formula presented) (other similar definitions may be found in the literature). Such formulations allow for solutions of the equation with discontinuous derivatives (as in the case of a moving contact line) where the solution goes to zero
-
An example of a weak form of Eq. (2) satisfies (Formula presented) for any sufficiently smooth test function (Formula presented) where the integrals are over all time and space. This expression is obtained by multiplying Eq. (2) by (Formula presented) and integrating twice by parts with no-flow boundary conditions, (Formula presented) (other similar definitions may be found in the literature). Such formulations allow for solutions of the equation with discontinuous derivatives (as in the case of a moving contact line) where the solution goes to zero.
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L. Sirovich, Applied Mathematical Sciences Vol. 100 Springer-Verlag, New York
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85035294243
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Calculations with such small (Formula presented)’s are not computationally too expensive since, for instance, the average time step (Formula presented) for (Formula presented) is approximately only (Formula presented) smaller than for (Formula presented)
-
Calculations with such small (Formula presented)’s are not computationally too expensive since, for instance, the average time step (Formula presented) for (Formula presented) is approximately only (Formula presented) smaller than for (Formula presented)
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