Randy C. Paffenroth
Worcester Polytechnic Institute
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Featured researches published by Randy C. Paffenroth.
International Journal of Bifurcation and Chaos | 2007
Eusebius J. Doedel; Volodymyr A. Romanov; Randy C. Paffenroth; Herbert B. Keller; D. J. Dichmann; Jorge Galán-Vioque; André Vanderbauwhede
We present an overview of detailed computational results for families of periodic orbits that emanate from the five libration points in the Circular Restricted 3-Body Problem, as well as for various secondary bifurcating families. Our extensive overview covers all values of the mass-ratio parameter, and includes many known families that have been studied in the past. The numerical continuation and bifurcation algorithms employed in our study are based on boundary value techniques, as implemented in the numerical continuation and bifurcation software AUTO.
International Journal of Bifurcation and Chaos | 2003
Eusebius J. Doedel; Randy C. Paffenroth; Herbert B. Keller; D. J. Dichmann; Jorge Galán-Vioque; André Vanderbauwhede
We show how to compute families of periodic solutions of conservative systems with two-point boundary value problem continuation software. The computations include detection of bifurcations and corresponding branch switching. A simple example is used to illustrate the main idea. Thereafter we compute families of periodic solutions of the circular restricted 3-body problem. We also continue the figure-8 orbit recently discovered by Chenciner and Montgomery, and numerically computed by Simo, as the mass of one of the bodies is allowed to vary. In particular, we show how the invariances (phase-shift, scaling law, and x, y, z translations and rotations) can be dealt with. Our numerical results show, among other things, that there exists a continuous path of periodic solutions from the figure-8 orbit to a periodic solution of the restricted 3-body problem.
Journal of Computational Physics | 2009
Oscar P. Bruno; Tim Elling; Randy C. Paffenroth; Catalin Turc
We present a new class of integral equations for the solution of problems of scattering of electromagnetic fields by perfectly conducting bodies. Like the classical Combined Field Integral Equation (CFIE), our formulation results from a representation of the scattered field as a combination of magnetic- and electric-dipole distributions on the surface of the scatterer. In contrast with the classical equations, however, the electric-dipole operator we use contains a regularizing operator; we call the resulting equations Regularized Combined Field Integral Equations (CFIE-R). Unlike the CFIE, the CFIE-R are Fredholm equations which, we show, are uniquely solvable; our selection of coupling parameters, further, yields CFIE-R operators with excellent spectral distributions-with closely clustered eigenvalues-so that small numbers of iterations suffice to solve the corresponding equations by means of Krylov subspace iterative solvers such as GMRES. The regularizing operators are constructed on the basis of the single layer operator, and can thus be incorporated easily within any existing surface integral equation implementation for the solution of the classical CFIE. We present one such methodology: a high-order Nystrom approach based on use of partitions of unity and trapezoidal-rule integration. A variety of numerical results demonstrate very significant gains in computational costs that can result from the new formulations, for a given accuracy, over those arising from previous approaches.
Siam Journal on Applied Dynamical Systems | 2002
Kathleen Hoffman; Robert S. Manning; Randy C. Paffenroth
We consider the problem of minimizing the energy of an inextensible elastic strut with length 1 subject to an imposed twist angle and force. In a standard calculus of variations approach, one first locates equilibria by solving the Euler--Lagrange ODE with boundary conditions at arclength values 0 and 1. Then one classifies each equilibrium by counting conjugate points, with local minima corresponding to equilibria with no conjugate points. These conjugate points are arclength values
IEEE Journal of Selected Topics in Signal Processing | 2013
Randy C. Paffenroth; Philip C. Du Toit; Ryan Nong; Louis L. Scharf; Anura P. Jayasumana; Vidarshana W. Bandara
\sigma \le 1
Journal of Physical Chemistry B | 2013
Christopher P. Calderon; Michael A. Thompson; Jason M. Casolari; Randy C. Paffenroth; W. E. Moerner
at which a second ODE (the Jacobi equation) has a solution vanishing at 0 and
Proceedings of SPIE | 2012
Randy C. Paffenroth; Philip C. Du Toit; Louis L. Scharf; Anura P. Jayasumana; Vidarshana W. Banadara; Ryan Nong
\sigma
International Journal of Bifurcation and Chaos | 1997
John H. Maddocks; Robert S. Manning; Randy C. Paffenroth; Kathleen A. Rogers; Jeremy A. Warner
.Finding conjugate points normally involves the numerical solution of a set of initial value problems for the Jacobi equation. For problems involving a parameter
Proceedings of SPIE, the International Society for Optical Engineering | 2008
Stephanie Chan; Randy C. Paffenroth
\lambda
2017 Cognitive Communications for Aerospace Applications Workshop (CCAA) | 2017
Paulo Victor Rodrigues Ferreira; Randy C. Paffenroth; Alexander M. Wyglinski; Timothy M. Hackett; Sven G. Bilén; Richard C. Reinhart; Dale J. Mortensen
, such as the force or twist angle in the elastic strut, this computation must be repeated for every value of