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In this paper, an analytical formulation of the system output is explicitly developed and directly used in order to determine solutions to the inversion problem.
In order to determine solutions of the initial-boundary-value problem (9 - 13), we use the Laplace transform with respect to variable t [29].
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Pure resistive SFCL and hybrid resistive SFCL were compared in order to determine suitable solutions for electric power systems.
Furthermore, multi-objective exergoeconomic optimization is performed using a genetic algorithm based on hybrid techniques in order to determine optimum solutions.
In order to determine feasible solutions for the problem, which appears to be a hard task for general-purpose solvers, we also develop and compare two metaheuristic approaches, namely a Tabu Search and a Variable Neighborhood Search algorithm.
In order to determine weak solutions of (1.3) in a suitable functional space E, we look for critical points of the functional J : E → R defined by J ( v ) = 1 p ∫ R N A ( x, v ) | ∇ v | p d x + 1 p ∫ R N ( b ( x ) − λ ) | v | p d x − ∫ R N F ( x, v ) d x, ∀ v ∈ E, (1.4).
In order to determine the solution of this equation, we first need to determine the solution of the following differential equation: D t m u ( x, t ) = F ( u, ∂ u ∂ x ⋯ ∂ n u ∂ x n, x, t ), t > 0, (2).
In order to determine the solution of this equation, we first need to determine the solution of the following differential equation: F ( u, D t k u, D x m u, x, t ) = 0, t > 0, (12).
In order to determine the solution of this equation, we first need to determine the solution of the following differential equation: D x m u ( x, t ) = F ( u, ∂ u ∂ t ⋯ ∂ n u ∂ t n, x, t ), t > 0, (7).
We introduce one more arbitrary boundary condition in addition to the boundary conditions (42) and (43) in order to determine the solution.
In order to determine the solution of initial-boundary values problem (9), (11 1,2, (12 2 and (13), we first take the Laplace transform [25] of Equation (9) and obtain q V ̄ ( y, q ) + λ q 2 V ̄ ( y, q ) = ν 1 + λ r q ∂ 2 V ̄ ( y, q ) ∂ y 2, (14).
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