Electromagnetic Analysis Using Transmission Line Variables. (Record no. 2929)
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| 000 -LEADER | |
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| fixed length control field | 11082nam a22004933i 4500 |
| 001 - CONTROL NUMBER | |
| control field | EBC5233517 |
| 003 - CONTROL NUMBER IDENTIFIER | |
| control field | MiAaPQ |
| 005 - DATE AND TIME OF LATEST TRANSACTION | |
| control field | 20260623164944.0 |
| 006 - FIXED-LENGTH DATA ELEMENTS--ADDITIONAL MATERIAL CHARACTERISTICS | |
| fixed length control field | m o d | |
| 007 - PHYSICAL DESCRIPTION FIXED FIELD--GENERAL INFORMATION | |
| fixed length control field | cr cnu|||||||| |
| 008 - FIXED-LENGTH DATA ELEMENTS--GENERAL INFORMATION | |
| fixed length control field | 260525s2017 xx o ||||0 eng d |
| 020 ## - INTERNATIONAL STANDARD BOOK NUMBER | |
| International Standard Book Number | 9789813225046 |
| Qualifying information | (electronic bk.) |
| 020 ## - INTERNATIONAL STANDARD BOOK NUMBER | |
| Canceled/invalid ISBN | 9789813225022 |
| 035 ## - SYSTEM CONTROL NUMBER | |
| System control number | (MiAaPQ)EBC5233517 |
| 035 ## - SYSTEM CONTROL NUMBER | |
| System control number | (Au-PeEL)EBL5233517 |
| 035 ## - SYSTEM CONTROL NUMBER | |
| System control number | (CaPaEBR)ebr11502265 |
| 035 ## - SYSTEM CONTROL NUMBER | |
| System control number | (OCoLC)1020286075 |
| 040 ## - CATALOGING SOURCE | |
| Original cataloging agency | MiAaPQ |
| Language of cataloging | eng |
| Description conventions | rda |
| -- | pn |
| Transcribing agency | MiAaPQ |
| Modifying agency | MiAaPQ |
| 050 #4 - LIBRARY OF CONGRESS CALL NUMBER | |
| Classification number | QC665.E4 .W456 2018 |
| 082 0# - DEWEY DECIMAL CLASSIFICATION NUMBER | |
| Classification number | 530.14/1 |
| 100 1# - MAIN ENTRY--PERSONAL NAME | |
| Personal name | Weiner, Maurice. |
| 245 10 - TITLE STATEMENT | |
| Title | Electromagnetic Analysis Using Transmission Line Variables. |
| 250 ## - EDITION STATEMENT | |
| Edition statement | 1st ed. |
| 264 #1 - PRODUCTION, PUBLICATION, DISTRIBUTION, MANUFACTURE, AND COPYRIGHT NOTICE | |
| Place of production, publication, distribution, manufacture | Singapore : |
| Name of producer, publisher, distributor, manufacturer | World Scientific Publishing Company, |
| Date of production, publication, distribution, manufacture, or copyright notice | 2017. |
| 264 #4 - PRODUCTION, PUBLICATION, DISTRIBUTION, MANUFACTURE, AND COPYRIGHT NOTICE | |
| Date of production, publication, distribution, manufacture, or copyright notice | �2018. |
| 300 ## - PHYSICAL DESCRIPTION | |
| Extent | 1 online resource (653 pages) |
| 336 ## - CONTENT TYPE | |
| Content type term | text |
| Content type code | txt |
| Source | rdacontent |
| 337 ## - MEDIA TYPE | |
| Media type term | computer |
| Media type code | c |
| Source | rdamedia |
| 338 ## - CARRIER TYPE | |
| Carrier type term | online resource |
| Carrier type code | cr |
| Source | rdacarrier |
| 505 0# - FORMATTED CONTENTS NOTE | |
| Formatted contents note | Intro -- Contents -- Preface -- NOTES ON THIRD EDITION -- 1. INTRODUCTION TO TRANSMISSION LINES AND THEIR APPLICATION TO ELECTROMAGNETIC PHENOMENA -- 1.1 Simple Experimental Example -- 1.2 Examples of Impulse Sources -- 1.3 Model Outline -- 1.4 Application of Model to Small Node Resistance -- 1.5 Transmission Line Theory Background -- 1.6 Initial Conditions of Special Interest -- One Dimensional TLM Analysis. Comparison with Finite Difference Method -- 1.7 TLM Iteration Method -- 1.8 Reverse TLM Iteration -- 1.9 Derivation of Scattering Coefficients For Reverse Iteration -- 1.10 Complete TLM Iteration (Combining Forward and Reverse Iterations) -- 1.11 Finite Difference Method. Comparison with TLM Method -- Two Dimensional TLM Analysis. Comparison With Finite Difference Method -- 1.12 Boundary Conditions at 2D Node -- 1.13 Static Behavior About 2D Node -- 1.14 Non-Static Example: Wave Incident on 2D Node -- 1.15 Integral Rotational Properties of Field About the Node -- 1.16 2D TLM Iteration Method for Nine Cell Core Matrix -- 1.17 2D Finite Difference Method. Comparison with TLM Method -- 1.18 Final comments: Inclusion of Time Varying Signals and Phase Coherence -- Appendices -- App. 1A.1 Effect of Additional Paths on Weighing Process -- App. 1A.2 Novel Applications of TLM Method: Description of Neurological Activity Using the TLM Method -- REFERENCES -- 2. NOTATION AND MAPPING OF PHYSICAL PROPERTIES -- 2.1 1D Cell Notation and Mapping of Conductivity and Field -- 2.2 Neighboring 1D Cells with Unequal Impedance -- 2.3 2D Cell Notation. Mapping of Conductivity and Field -- 2.4 Simultaneous Conductivity Contributions -- 2.5 3D Cell Notation. Mapping of Conductivity and Field -- Other Node Controlled Properties -- 2.6 Node Control of 2D Scattering Coefficients Due to Finite Node Resistance -- 2.7 Signal Gain. |
| 505 8# - FORMATTED CONTENTS NOTE | |
| Formatted contents note | 2.8 Signal Generation. Use of Node Coupling -- 2.9 Mode Conversion -- Example of Mapping: Node Resistance in Photoconductive Semiconductor -- 2.10 Semiconductor Switch Geometry (2D) and Model -- 2.11 Node Resistance Profile in Semiconductor -- 3. SCATTERING EQUATIONS -- 3.1 1D Scattering Equations -- 3.2 2D Scattering Equations -- 3.3 Effect of Symmetry on Scattering Coefficients -- 3.4 3D Scattering Equations: Coplanar Scattering -- General Scattering, Including Scattering Normal to the Propagation Plane -- 3.5 Simple 3D Equivalent TLM Circuit -- 3.6 Quasi-Coupling -- 3.7 Neglect of Quasi-Coupling -- 3.8 Simple Quasi-Coupling Circuit: First Order Approximation -- 3.9 Correction to Quasi-Coupling Circuit: Second Order Approximation -- 3.10 Calculation of Load Impedance with Quasi-Coupling -- 3.11 Small Coupling Approximation of Second Order Quasi-Coupling -- 3.12 General 3D Scattering Process Using Cell Notation -- 3.13 Complete Iterative Equations -- 3.14 Contribution of Electric and Magnetic Fields to Total Energy -- Plane Wave Behavior -- 3.15 Response of 2D Cell Matrix to Input Plane Wave -- 3.16 Response of 2D Cell Matrix to Input Waves with Arbitrary Amplitudes -- 3.17 Response of 3D Cell Matrix to Input Plane Wave -- 3.18 Final Comments of Uniform Waves Versus Plane Waves -- Appendices -- App.3A.1 Consistency of 3D Circuit with the TLM Static Solutions -- App.3A.2 3D Scattering Coefficients, Without Quasi-Coupling In Terms of Circuit Parameters -- App.3A.3 3D Scattering Coefficients with Both Coplanar and Aplanar Contributions into Unit Cell Lines -- App.3A.4 3D Scattering Equations: with Both Coplanar and Aplanar Contributions into Unit Cell Lines -- 4. CORRECTIONS FOR PLANE WAVE AND GRID ANISOTROPY EFFECTS -- 4.1 Partition of TLM Waves into Component Waves -- How do we Treat a Sign Disparity in +VA and +VB ?. |
| 505 8# - FORMATTED CONTENTS NOTE | |
| Formatted contents note | 4.2 Plane Wave Correlation Models Between Cells (2D). Local and Long Range Models and Their Effect on Scattering -- 4.3 Three Cell Correlation Model -- 4.4 Incorporation of Correlation Coefficients (3-Cell Model) -- 4.5 Description of TLM Wave Packet Using the 3-Cell Model with Correlation Coefficients. Modification Adjacent a Low Density State -- 4.6 Composite Model Incorporating Correlation Coefficients. Application to a Plane Wave Packet Including Decorrelation Examples -- Distinction Between Correlation and Decorrelation Processes -- Useful Relations for � Values Close to Unity -- Underlying Physics of Decorrelation Coefficients and Their Effect on the Properties of Coherent Plane Wave Fronts -- 4.7 Changes to 2D Scattering Coefficients for Partitioned Waves -- Corrections to Plane Wave Correlations/Decorrelations -- 4.8 Wave Correlations with Differing Dielectric Interface -- 4.9 Wave Correlations with a Conductor/Dielectric Interface -- 4.10 Use of Correlation Coefficients to Treat Boundaries -- 4.11 Plane Wave Incident on a Half-Infinite Conducting Plane in Terms of Both the 3-Cell and Composite Models -- Sign Disparity and Opposing Plane Wave Decorrelations -- 4.12 Decorrelation Due to Sign Disparity of Plane and Symmetric Waves -- The Need to Decorrelate an Incoming Plane Wave When a Sign Disparity Results -- Various Techniques and Approximations for Removing Sign Disparities -- Summary of Approximations I-V For Removing Sign Disparities -- 4.13 Related Scattering Criteria and Necessary Conditions for Removing the Sign Disparities -- 4.14 Decorrelation of Forward and Backward (Opposing) Plane Waves with Same Polarity (Phase) in TLM Lines without Losses -- 4.15 Summary of Correlation/Decorrelation Coefficients. Possible Reduction in the Number of Coefficients. |
| 505 8# - FORMATTED CONTENTS NOTE | |
| Formatted contents note | 4.16 Use of the Various Coefficients in Least Action Solutions. Why is the Least Action Method desirable? -- 4.17 Possible Experimental Arrangements for Determination of the Correlation/Decorrelation Coefficients -- 4.18 Flow Diagram of Various Processes -- Treatment of Grid Orientation Effects -- 4.19 Dependence of Wave Energy Dispersal on Grid Orientation for Symmetric and Plane Waves -- 4.20 Use of Principal Grids for Plane Wave Propagation -- 4.21 Transformation Properties Between Grids -- 4.22 Principal Grids and Mini-Plane Wave Fronts Associated with Each Cell. Plane Wave Partitioning -- Co-Existence of Principal Propagation Vectors in all Quadrants. Modification of Principal Vector -- 4.23 Transformation of Fields to the Principal Grid -- 4.24 Incorporation of Symmetric Waves into a Principal Grid -- 4.25 Iteration Method Using Principal Grid Transformations -- 4.26 Final Comments -- Appendices -- App.4A.1 3D Scattering Corrections of Plane Waves (Plane Wave Correlations Using 3-Cell Model) -- App.4A.2 Consistency of Plane Wave Correlations With a Quantum Mechanical Model -- Decorrelation Examples: 1) Photon Transitions between States Due to Presence of Density Gradients, and 2) Wave Obstructions -- App. 4A.3 Linkage of the Composite Correlation Model to the Quantum Mechanics. Decorrelations Due to Residual Symmetric Waves -- Other Quantum Related Decorrelation Processes Apps. (4A.4a-4A.4c) -- App. 4A.4a Decorrelation Effects of Opposing Waves Using QM Notation -- App. 4A.4b Decorrelation Effects Due to Sign Disparities Using QM Notation -- App. 4A.4c Decorrelation due to an Obstruction (Quantum Viewpoint) -- App. 4A.4d Selection of the Number of m States for Simulations -- App.4A.5 Least Action Solution Methods for Removing Sign Disparities -- 5. BOUNDARY CONDITIONS AND DISPERSION -- 5.1 Dielectric-Dielectric Interface. |
| 505 8# - FORMATTED CONTENTS NOTE | |
| Formatted contents note | Node Coupling: Nearest Node And Multi-Coupled Node Approximations -- 5.2 Nearest Nodes for 1D Interface -- 5.3 Nearest Nodes at 2D Interface -- 5.4 Truncated Cells and Oblique Interface -- 5.5 Cell Index Notation at a Dielectric Interface Used in Simulations -- 5.6 Simplified Iteration Neglecting the Nearest Node Approximation -- 5.7 Non-Uniform Dielectric. Use of Cluster Cells -- Other Boundary Conditions -- 5.8 Dielectric - Open Circuit Interface -- 5.9 Dielectric - Conductor Interface -- 5.10 Input/Output Conditions -- 5.11 Composite Transmission Line -- 5.12 Determination of Initial Static Field by TLM Method -- Dispersion -- 5.13 TLM Methods for Treating Dispersion -- 5.14 Dispersion Sources -- 5.15 Dispersion Example -- 5.16 Propagation Velocity Dispersion -- 5.17 Node Resistance Dispersion -- 5.18 Anomalous Dispersion -- Incorporation of Dispersion into TLM Formulation -- 5.19 Dispersion Approximations -- 5.20 Outline of Dispersion Calculation Using the TLM Method -- 5.21 One Dimensional Dispersion Iteration -- 5.22 Initial Conditions with Dispersion Present -- 5.23 Stability of Initial Profiles with Dispersion Present -- 5.24 Replacement of Non-Uniform Field with an Effective Uniform Field -- Appendix -- App.5A.1 Specification of Input/Output Node Resistance to Eliminate Multiple Reflections -- REFERENCES -- 6. CELL DISCHARGE PROPERTIES AND INTEGRATION OF TRANSPORT PHENOMENA INTO THE TRANSMISSION LINE MATRIX -- 6.1 Charge Transfer Between Cells -- 6.2 Relationship Between Field and Cell Charge -- 6.3 Dependence of Conductivity on Carrier Properties -- Integration of Carrier Transport Using TLM Notation. Changes in Cell Occupancy and Its Effect on the TLM Iteration -- 6.4 General Continuity Equations -- 6.5 Carrier Generation Due to Light Activation -- 6.6 Carrier Generation Due to Avalanching: Identical Hole and Electron Drift Velocities. |
| 505 8# - FORMATTED CONTENTS NOTE | |
| Formatted contents note | 6.7 Avalanching with Differing Hole and Electron Drift Velocities. |
| 588 ## - SOURCE OF DESCRIPTION NOTE | |
| Source of description note | Description based on publisher supplied metadata and other sources. |
| 590 ## - LOCAL NOTE (RLIN) | |
| Local note | Electronic reproduction. Ann Arbor, Michigan : ProQuest Ebook Central, 2026. Available via World Wide Web. Access may be limited to ProQuest Ebook Central affiliated libraries. |
| 650 #0 - SUBJECT ADDED ENTRY--TOPICAL TERM | |
| Topical term or geographic name entry element | Electromagnetic fields-Mathematics. |
| 655 #4 - INDEX TERM--GENRE/FORM | |
| Genre/form data or focus term | Electronic books. |
| 776 08 - ADDITIONAL PHYSICAL FORM ENTRY | |
| Relationship information | Print version: |
| Main entry heading | Weiner, Maurice |
| Title | Electromagnetic Analysis Using Transmission Line Variables |
| Place, publisher, and date of publication | Singapore : World Scientific Publishing Company,c2017 |
| International Standard Book Number | 9789813225022 |
| 797 2# - LOCAL ADDED ENTRY--CORPORATE NAME (RLIN) | |
| Corporate name or jurisdiction name as entry element | ProQuest (Firm) |
| 856 40 - ELECTRONIC LOCATION AND ACCESS | |
| Uniform Resource Identifier | <a href="https://ebookcentral-proquest-com.mlisicats.remotexs.co/lib/ppks/detail.action?docID=5233517">https://ebookcentral-proquest-com.mlisicats.remotexs.co/lib/ppks/detail.action?docID=5233517</a> |
| Public note | Click to View |
| 942 ## - ADDED ENTRY ELEMENTS (KOHA) | |
| Source of classification or shelving scheme | Library of Congress Classification |
| Koha item type | E-Book |
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