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The Oblique Derivative Problem for the Laplace Equation in a Plain Domain
Authors:Email author" target="_blank">Dagmar?MedkováEmail author
Institution:(1) Mathematical Institute, Czech Academy of Sciences, Zcaronitná 25, 115 67 Praha 1, Czech Republic;(2) Faculty of Mechanical Engineering, Department of Technical Mathematics, Czech Technical University, Karlovo nám. 13, 121 35 Praha 2, Czech Republic
Abstract:The oblique derivative problem for the Laplace equation is studied in a planar multiply connected domain. The boundary condition has a form 
	$$(n + \beta\tau)\cdot \nabla u = g$$
	where 
	$$n$$
	is the unit normal vector, 
	$$\tau$$
	is the unit tangential vector and 
	$$\beta$$
	is a fixed real number. If 
	$$g$$
	is a Hölderian function and the corresponding domain has Ljapunov boundary then the classical problem is studied. If 
	$$g \in L_p$$
	on the boundary and the domain has a locally Lipschitz boundary then a solution, which fulfils the boundary condition in the sense of a nontangential limit, is studied. If 
	$$g$$
	is a real measure on the boundary and the domain has bounded cyclic variation then a solution in a sense of distributions is studied. The solution is looked for in a form of a linear combination of a single layer potential and an angular potential.
Keywords:Primary: 35J05  Secondary: 31A10
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