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Robert J. Martin

dblp:129/5959 · DBLP profile ↗
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1ranked-venue papers
1as first author
0since 2021 · last 1960
—ORCID · none

Domains — the database's venue-derived domains; a paper can count in several

Systems, architecture and hardware · 1 · 1 first-author

Expertise — from the expertise taxonomy: the topics of the expert's papers under the CCF categories. A weight counts papers with recency: 1 for a paper about the topic, 0.3 when the topic is its context, halved every five years.

Interdisciplinary, comprehensive, and emerging computing
1 paper
Computational science and engineering · 100%
Computer architecture, parallel and distributed computing, and storage systems
1 paper
Integrated circuit design · 100%

Topics — the 3 heaviest of 3, each with the papers that count most for it

TopicWeightPapersLastEvidence papers
Integrated circuit design › analog and mixed-signal circuits
analog circuit design
0.011960
Analog Representation of Poisson's Equation in Two Dimensions · IRE Trans. Electron. Comput. 1960
Computational science and engineering
partial differential equation solver
0.011960
Analog Representation of Poisson's Equation in Two Dimensions · IRE Trans. Electron. Comput. 1960
Computational science and engineering › partial differential equations
poisson's equation
0.011960
Analog Representation of Poisson's Equation in Two Dimensions · IRE Trans. Electron. Comput. 1960
YearPublicationVenuePosition
1960 Analog Representation of Poisson's Equation in Two Dimensions
abstract
A new analog device, called a Poisson cell, has been developed which aids in obtaining solutions to either Laplace's equation or Poisson's equation. The cell may be used to simulate such potentials as electric potential, magnetic potential, gravitational potential, and the velocity potential of irrotational flow; it has applications in the fields of hydrodynamics, heat conduction, and aerodynamics. The cell is a solid volume-conducting medium made from a homogeneous mixture of hydrostone and graphite. Electrode configurations may be painted on the surface with conducting paint or imbedded directly in the structure. In the case of Poisson's equation, where ∇2ø(x, y) = f(x, y), the function f(x, y) is simulated by injecting currents into the underside of the cell. The application of the Poisson cell to numerous problems and in particular to problems in electron flow is discussed m detail, along with the incorporation of the cell into either an analog computer system or a combined analog-digital computer system.
Robert J. Martin, Nino A. Masnari, Joseph E. Rowe
IRE Trans. Electron. Comput.1