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- W108001666 abstract "Thomson W. and Tait P. were the first who applied the Hamilton principle to the fluid [1,2] $$intlimits_{{{{t}_{1}}}}^{{{{t}_{2}}}} delta Ldt = intlimits_{{{{t}_{1}}}}^{{{{t}_{2}}}} {dt} intlimits_{{partial Omega }} {p{{delta }_{n}}} bullet ,dS, {{delta }_{n}}({{t}_{1}}) = {{delta }_{n}}({{t}_{2}}) = 0, $$(1.1)Where δn is the virtual displacement of fluid flow boundary ∂Ω, the integral represents the work of the force of fluid pressure p on the displacement δn, L is the functional of the boundary and the normal velocity (the Lagrange function)." @default.
- W108001666 created "2016-06-24" @default.
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- W108001666 date "1992-01-01" @default.
- W108001666 modified "2023-09-24" @default.
- W108001666 title "Incompressible Fluid Flows with Free Boundary and the Methods for their Research" @default.
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- W108001666 doi "https://doi.org/10.1007/978-3-0348-8627-7_28" @default.
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