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EMPHASIS(TM)/Nevada CABANA User Guide Version 2.1.1

Turner, C.D.; Bohnhoff, William J.; Troup, Jennifer L.

The CABle ANAlysis (CABANA) portion of the EMPHASIS(TM) suite is designed specifically for the simulation of cable SGEMP. The code can be used to evaluate the response of a specific cable design to threat or to compare and minimize the relative response of difference d esigns. This document provides user - specific information to facilitate the application of the code to cables of interest. Acknowledgement The authors would like to thank all of those individuals who have helped to bring CABANA to the point it is today, including Gary Scrivner and Wesley Fan for many useful theory and design discussions.

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TYPE SAND Report YEAR 2014
OSTIDOI

EMPHASIS/Nevada CABANA user Guide. Version 2.0

Turner, C.D.; Bohnhoff, William J.; Troup, Jennifer L.

The CABle ANAlysis (CABANA) portion of the EMPHASIS{trademark} suite is designed specifically for the simulation of cable system-generated electromagnetic pulse (SGEMP). The code can be used to evaluate the response of a specific cable design to threat or to compare and minimize the relative response of difference designs. This document provides user-specific information to facilitate the application of the code to cables of interest. It solves the electrical portion of a cable SGEMP simulation. It takes specific results from the deterministic radiation-transport code CEPTRE as sources and computes the resulting electrical response to an arbitrary cable load. The cable geometry itself is also arbitrary and is limited only by the patience of the user in meshing and by the available computing resources for the solution. The CABANA simulation involves solution of the quasi-static Maxwell equations using finite-element method (FEM) techniques.

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TYPE SAND Report YEAR 2011
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Discrete Ordinates Approximations to the First- and Second-Order Radiation Transport Equations

Fan, Wesley C.; Drumm, Clifton R.; Troup, Jennifer L.

The conventional discrete ordinates approximation to the Boltzmann transport equation can be described in a matrix form. Specifically, the within-group scattering integral can be represented by three components: a moment-to-discrete matrix, a scattering cross-section matrix and a discrete-to-moment matrix. Using and extending these entities, we derive and summarize the matrix representations of the second-order transport equations.

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TYPE Report YEAR 2002
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19 Results
19 Results