Publications

Cyr, Eric C.; Miller, Sean M.; Pawlowski, Roger P.; Phillips, Edward G.; Beckwith, Kristian B.; Bettencourt, Matthew T.; Cartwright, Keith C.; Kramer, Richard M.; Roberts, Nathan V.; Shadid, John N.; Shields, Sidney S.

Abstract not provided.

Cyr, Eric C.; Miller, Sean M.; Phillips, Edward G.; Beckwith, Kristian B.; Bettencourt, Matthew T.; Cartwright, Keith C.; Kramer, Richard M.; Pawlowski, Roger P.; Roberts, Nathan V.; Shadid, John N.; Shields, Sidney S.

Abstract not provided.

Bettencourt, Matthew T.; Shields, Sidney S.; Beckwith, Kristian B.; Cartwright, Keith C.; Cyr, Eric C.; Kramer, Richard M.; Lin, Paul L.; McDoniel, William M.; Miller, Sean M.; Pawlowski, Roger P.; Phillips, Edward G.; Roberts, Nathan V.

Abstract not provided.

Cartwright, Keith C.; Bettencourt, Matthew T.; Pointon, Timothy D.; Beckwith, Kristian B.; Cyr, Eric C.; Kramer, Richard M.; McDoniel, William M.; Miller, Sean M.; Radtke, Gregg A.; Shields, Sidney S.; Swan, Matthew S.; Turner, C.D.; Moore, Christopher H.

Abstract not provided.

Cyr, Eric C.; Beckwith, Kristian B.; Bettencourt, Matthew T.; Cartwright, Keith C.; Kramer, Richard M.; Miller, Sean T.; Pawlowski, Roger P.; Phillips, Edward G.; Roberts, Nathan V.; Shadid, John N.

Abstract not provided.

Bettencourt, Matthew T.; Kramer, Richard M.; Cartwright, Keith C.; Phillips, Edward G.; Ober, Curtis C.; Pawlowski, Roger P.; Swan, Matthew S.; Kalashnikova, Irina; Phipps, Eric T.; Conde, Sidafa C.; Cyr, Eric C.; Ulmer, Craig D.; Kordenbrock, Todd H.; Levy, Scott L.; Templet, Gary J.; Hu, Jonathan J.; Lin, Paul L.; Glusa, Christian A.; Siefert, Christopher S.; Glass, Micheal W.

This report documents the outcome from the ASC ATDM Level 2 Milestone 6358: Assess Status of Next Generation Components and Physics Models in EMPIRE. This Milestone is an assessment of the EMPIRE (ElectroMagnetic Plasma In Realistic Environments) application and three software components. The assessment focuses on the electromagnetic and electrostatic particle-in-cell solu- tions for EMPIRE and its associated solver, time integration, and checkpoint-restart components. This information provides a clear understanding of the current status of the EMPIRE application and will help to guide future work in FY19 in order to ready the application for the ASC ATDM L 1 Milestone in FY20. It is clear from this assessment that performance of the linear solver will have to be a focus in FY19.

Journal of Computational Physics

Kramer, Richard M.; Siefert, Christopher S.; Voth, Thomas E.; Bochev, Pavel B.

A discrete De Rham complex enables compatible, structure-preserving discretizations for a broad range of partial differential equations problems. Such discretizations can correctly reproduce the physics of interface problems, provided the grid conforms to the interface. However, large deformations, complex geometries, and evolving interfaces makes generation of such grids difficult. We develop and demonstrate two formally equivalent approaches that, for a given background mesh, dynamically construct an interface-conforming discrete De Rham complex. Both approaches start by dividing cut elements into interface-conforming subelements but differ in how they build the finite element basis on these subelements. The first approach discards the existing non-conforming basis of the parent element and replaces it by a dynamic set of degrees of freedom of the same kind. The second approach defines the interface-conforming degrees of freedom on the subelements as superpositions of the basis functions of the parent element. These approaches generalize the Conformal Decomposition Finite Element Method (CDFEM) and the extended finite element method with algebraic constraints (XFEM-AC), respectively, across the De Rham complex.

McGregor, Duncan A.; Love, Edward L.; Kramer, Richard M.

We investigate the use of implicit time integrators for finite element time domain approximations of Maxwell's equations in vacuum. We discretize Maxwell's equations in time using Crank-Nicolson and in 3D space using compatible finite elements. We solve the system by taking a single step of Newton's method and inverting the Eddy-Current Schur complement allowing for the use of standard preconditioning techniques. This approach also generalizes to more complex material models that can include the Unsplit PML. We present verification results and demonstrate performance at CFL numbers up to 1000.

Turner, C.D.; Pasik, Michael F.; Seidel, David B.; Pointon, Timothy D.; Cartwright, Keith C.; Kramer, Richard M.; McGregor, Duncan A.

The Unstructured Time-Domain ElectroMagnetics (UTDEM) portion of the EMPHASIS suite solves Maxwell’s equations using finite-element techniques on unstructured meshes. This document provides user-specific information to facilitate the use of the code for applications of interest.

Voth, Thomas E.; Mosso, Stewart J.; Kramer, Richard M.; Luchini, Christopher B.; Niederhaus, John H.

Abstract not provided.

Phillips, Edward G.; Bettencourt, Matthew T.; Cyr, Eric C.; Ellis, Truman E.; Kramer, Richard M.; McGregor, Duncan A.; Miller, Sean M.; Niederhaus, John H.; Shadid, John N.

Abstract not provided.

Fisher, Koa F.; Kramer, Richard M.; Voth, Thomas E.

Abstract not provided.

Kramer, Richard M.

Abstract not provided.

Bettencourt, Matthew T.; Cyr, Eric C.; Kramer, Richard M.; Miller, Sean M.; Pawlowski, Roger P.; Phillips, Edward G.; Robinson, Allen C.; Shadid, John N.

Abstract not provided.

Bettencourt, Matthew T.; Cyr, Eric C.; Kramer, Richard M.; Miller, Sean M.; Pawlowski, Roger P.; Phillips, Edward G.; Robinson, Allen C.; Shadid, John N.

Abstract not provided.

Miller, Sean M.; Niederhaus, John H.; Kramer, Richard M.; Radtke, Gregg A.

Abstract not provided.

Bettencourt, Matthew T.; Shadid, John N.; Cyr, Eric C.; Phillips, Edward G.; Kramer, Richard M.; Niederhaus, John H.; Robinson, Allen C.

Abstract not provided.

Kramer, Richard M.; Miller, Sean M.; Niederhaus, John H.; Radtke, Gregg A.; Bettencourt, Matthew T.; Cartwright, Keith C.; Cyr, Eric C.; Phillips, Edward G.; Robinson, Allen C.; Shadid, John N.

Abstract not provided.

Shadid, John N.; Phillips, Edward G.; Cyr, Eric C.; Pawlowski, Roger P.; Bettencourt, Matthew T.; Cartwright, Keith C.; Lin, Paul L.; Kramer, Richard M.; Niederhaus, John H.; Radtke, Gregg A.; Robinson, Allen C.

Abstract not provided.

Bettencourt, Matthew T.; Cyr, Eric C.; Pawlowski, Roger P.; Kramer, Richard M.; Phillips, Edward G.; Shadid, John N.; Robinson, Allen C.

Abstract not provided.

Bettencourt, Matthew T.; Cyr, Eric C.; Pawlowski, Roger P.; Kramer, Richard M.; Phillips, Edward G.; Shadid, John N.; Robinson, Allen C.

Abstract not provided.

Kramer, Richard M.; Noble, David R.

Interface-conforming elements generated by the conformal decomposition finite element method can have arbitrarily poor quality due to the arbitrary intersection of the base triangular or tetrahedral mesh with material interfaces. This can have severe consequences for both the solvability of linear systems and for the interpolation error of fields represented on these meshes. The present work demonstrates that snapping the base mesh nodes to the interface whenever the interface cuts close to a node results in conforming meshes of good quality. Theoretical limits on the snapping tolerance are derived, and even conservative tolerance choices result in limiting the stiffness matrix condition number to within a small multiple of that of the base mesh. Interpolation errors are also well controlled in the norms of interest. In 3D, use of node-to-interface snapping also permits a simpler and more robust vertex ID-based element decomposition algorithm to be used with no serious detriment to mesh quality.

Voth, Thomas E.; Sanchez, Jason J.; Mosso, Stewart J.; Kramer, Richard M.

Abstract not provided.

Noble, David R.; Kramer, Richard M.

Abstract not provided.

Kramer, Richard M.; Noble, David R.

Abstract not provided.