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Poisson kernel

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In mathematics, and specifically in potential theory, the Poisson kernel is an integral kernel, used for solving the two-dimensional Laplace equation, given Dirichlet boundary conditions on the unit disk. The kernel can be understood as the derivative of the Green's function for the Laplace equation. It is named for Siméon Poisson. Poisson kernels commonly find applications in control theory and two-dimensional problems in electrostatics.

Fourier transformFourier transformMathematical transform that expresses a function of time as a function of frequencyThe Fourier transform applied to the waveform of a C majorpianochord (with logarithmic horizontal (frequency) axis). The first three peaks on the left correspond to the fundamental frequencies of the chord (C, E, G).Complex planeComplex planeThe complex plane. The horizontal axis represents the real numbers(R){\displaystyle (\mathbb {R} )}, the vertical axis represents the imaginary numbers(I){\displaystyle (\mathbb {I} )}.Banach spaceIn mathematics, more specifically in functional analysis, a Banach space (, Polish pronunciation: [ˈba.nax]) is a complete normed vector space. Thus, a Banach space is a vector space with a metric that allows the computation of vector length and distance between vectors and is complete in the sense that a Cauchy sequence of vectors always converges to a well-defined limit that is within the space.Green's functionGreen's functionMethod of solution to differential equationsUnit diskUnit diskIn mathematics, the open unit disk (or disc) around P (where P is a given point in the plane), is the set of points whose distance from P is less than 1: D1(P)={Q:|P−Q|<1}.{\displaystyle D_{1}(P)=\{Q:\vert P-Q\vert <1\}.\,}The closed unit disk around P is the set of points whose distance from P is less than or equal to one: D¯1(P)={Q:|P−Q|≤1}.{\displaystyle {\bar {D}}_{1}(P)=\{Q:|P-Q|\leq 1\}.\,}Unit disks are special cases of disks and unit balls; as such, they contain the interior of the unit circle and, in the case of the closed unit disk, the unit circle itself.Dirichlet boundary conditionDirichlet boundary conditionType of constraint on solutions to differential equations Differential equations Scope Fields Natural sciencesEngineering Astronomy Physics Chemistry Biology Geology Applied mathematics Continuum mechanics Chaos theory Dynamical systems Social sciences Economics Population dynamics Classification Types Ordinary Partial Differential-algebraic Integro-differential Fractional Linear Non-linear By variable type Dependent and independent variables Autonomous Coupled / Decoupled Exact Homogeneous / Nonhomogeneous Features Order Operator Notation Relation to processes Difference (discrete analogue) Stochastic Stochastic partial Delay Solution Existence and uniqueness Well-posed problem Picard–Lindelöf theorem Peano existence theorem Carathéodory's existence theorem Cauchy–Kovalevskaya theorem General topics Initial values Boundary values Dirichlet Neumann Robin Cauchy Periodic Wronskian Abel's identity Sturm–Liouville theory Floquet theory Phase portrait Stability Lyapunov Asymptotic Exponential Series solutions Rate of convergence Asymptotic series Special functions Numerical integration Dirac delta function Solution methods Inspection Method of characteristics Ansatz Euler Exponential response formula Finite difference Crank–Nicolson Finite element Infinite element Finite volume Galerkin Petrov–Galerkin Green's function Integrating factor Integral transforms Perturbation theory Reduction of order Runge–Kutta Separation of variables Undetermined coefficients Variation of parameters WKB approximation People List Newton Leibniz Jacob Bernoulli d'Alembert Clairaut Euler Lagrange Laplace Wroński Fourier Cauchy Green Dirichlet Sturm Liouville Neumann Robin Boole Kovalevskaya Runge Kutta Lipschitz Lindelöf Picard Jeffreys Nicolson Crank Hrennikoff Courant Named equationsvte In mathematics, the Dirichlet boundary condition is imposed on an ordinary or partial differential equation, such that the values that the solution takes along the boundary of the domain are fixed.Potential theoryPotential theoryIn mathematics and mathematical physics, potential theory is the study of harmonic functions. The term "potential theory" dates from 19th-century physics when it was realized that the two fundamental forces of nature known at the time, namely gravity and the electrostatic force, could be modeled using functions called the gravitational potential and electrostatic potential, both of which satisfy Poisson's equation—or in the vacuum, Laplace's equation.Laplace's equationLaplace's equationIn mathematics and physics, Laplace's equation is a second-order partial differential equation named after Pierre-Simon Laplace, who first studied its properties in 1786.DerivativeDerivativeInstantaneous rate of change (mathematics)The graph of a function, drawn in black, and a tangent line to that graph, drawn in red. The slope of the tangent line is equal to the derivative of the function at the marked point.The derivative at different points of a differentiable function. In this case, the derivative is equal to ⁠sin⁡(x2)+2x2cos⁡(x2){\displaystyle \sin \left(x^{2} ight)+2x^{2}\cos \left(x^{2} ight)}⁠.Control theoryControl theoryControl theory is a field of control engineering and applied mathematics that deals with the control of dynamical systems. The aim is to develop a model or algorithm governing the application of system inputs to drive the system to a desired state, while minimizing any delay, overshoot, or steady-state error and ensuring a level of control stability; often with the aim to achieve a degree of optimality.Integral transformIntegral transformMapping involving integration between function spaces In mathematics, an integral transform is a type of transformation that maps a function from its original function space into another function space via integration, where some of the properties of the original function might be more easily characterized and manipulated than in the original function space. The transformed function can generally be mapped back to the original function space using the inverse transform.ElectrostaticsElectrostaticsElectrostatics is a branch of physics that studies slow-moving or stationary electric charges on macroscopic objects where quantum effects can be neglected. Under these circumstances, the electric field, electric potential, and the charge density are related without complications from magnetic effects. Since classical antiquity, it has been known that some materials, such as amber, attract lightweight particles after rubbing.

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