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On computation of capacities and conformal invariants

Mohamed M S Nasser, Matti Vuorinen

Abstract

We give a survey of computation of the conformal capacity of planar condensers, generalized capacity, and logarithmic capacity with emphasis on our recent work 2020-2025. We also discuss some applications of our method based on the boundary integral equation with the generalized Neumann kernel to the computation of several other conformal invariants: harmonic measure, modulus of a quadrilateral, reduced modulus, hyperbolic capacity, and elliptic capacity. Here the solution of mixed Dirichlet-Neumann boundary value problem for the Laplace equation has a key role. At the end of the paper we give a topicwise structured list to our extensive bibliography on constructive complex analysis and potential theory.

On computation of capacities and conformal invariants

Abstract

We give a survey of computation of the conformal capacity of planar condensers, generalized capacity, and logarithmic capacity with emphasis on our recent work 2020-2025. We also discuss some applications of our method based on the boundary integral equation with the generalized Neumann kernel to the computation of several other conformal invariants: harmonic measure, modulus of a quadrilateral, reduced modulus, hyperbolic capacity, and elliptic capacity. Here the solution of mixed Dirichlet-Neumann boundary value problem for the Laplace equation has a key role. At the end of the paper we give a topicwise structured list to our extensive bibliography on constructive complex analysis and potential theory.

Paper Structure

This paper contains 51 sections, 2 theorems, 151 equations, 16 figures, 2 tables.

Key Result

Theorem 3.1

For a given function $\gamma\in H$, there exits a unique function $\rho\in H$ and a unique piecewise constant function with real constants $\nu_0,\nu_1,\ldots,\nu_m$, such that the formula defines the boundary values of an analytic function $f$ in $G$ with $f(\infty)=0$ for unbounded $G$. The function $\rho$ is the unique solution of the integral equation and the piecewise constant function $\n

Figures (16)

  • Figure 1: The domains of the condensers considered in Examples \ref{['ex:sq']}, \ref{['ex:lens']}, and \ref{['ex:dpg']}.
  • Figure 2: The relative error in the computed values of the capacities of the condensers in Examples \ref{['ex:ring']} (left) and \ref{['ex:sq']} (right) where $n$ is the number of mesh points on each boundary component of $G$.
  • Figure 3: The computed values of the capacity of the condenser $(\Omega,E)$ in Examples \ref{['ex:dpg']} and the capacities of $(\Omega,\overline{B^2(0,r_k)})$, $k=1,2$.
  • Figure 4: Left: The computed values of the capacity of the condenser in Examples \ref{['ex:lens']}. Right: absolute values of the differences between the computed values of the capacity and the estimate \ref{['eq:len-est']}.
  • Figure 5: Left: The domain of the condenser in Examples \ref{['ex:7d']}. Right: The computed values of the constants $a_1,\ldots,a_7$ for $0.01\le r\le 0.17$.
  • ...and 11 more figures

Theorems & Definitions (27)

  • Theorem 3.1: nv1
  • Remark 3.1
  • Example 4.1: Circular ring
  • Example 4.2: Square in square: bsvps10p2
  • Example 4.3: Disk with a polygonal hole
  • Example 4.4: Lens shaped plate: hnv0mc
  • Example 4.5: A disk with $7$ circular holes
  • Example 5.1: Circular domain
  • Example 6.1: Hyperbolic capacity of an ellipse
  • Remark 6.1
  • ...and 17 more