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|a Kaufman, Alexander A.,
|d 1931-
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|a Basic principles of induction logging
|h [electronic resource] :
|b electromagnetic methods in borehole geophysics /
|c Alexander Kaufman, Gregory Itskovich
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| 260 |
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|a Amsterdam :
|b Elsevier,
|c 2017
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| 300 |
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|a 1 online resource (522 p.)
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| 500 |
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|a 3.1. Plane Wave in a Uniform Medium
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|a Front Cover; Basic Principles of Induction Logging: Electromagnetic Methods in Borehole Geophysics; Copyright; Dedication; Contents; Introduction; Acknowledgments; List of Symbols; Chapter One: System of Equations of the Stationary Electric and Magnetic Fields; 1.1. Equations of the Stationary Electric Field in a Conducting and Polarizable Medium; 1.2. Interaction of Currents, Biot-Savart Law, and Magnetic Field; 1.2.1. Ampere's Law and Interaction of Currents; 1.2.2. Magnetic Field and Biot-Savart Law; 1.2.3. Lorentz Force and Electromotive Force Acting on the Moving Circuit; Example One
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|a 1.5.4. Example Four: Magnetic Field Due to a Current in a Cylindrical Conductor1.5.5. Example Five: Magnetic Field of Infinitely Long Solenoid; 1.5.6. Example Six: Magnetic Field of a Current Toroid; 1.6. System of Equations for the Stationary Fields; References; Further Reading; Chapter Two: Physical Laws and Maxwell's Equations; 2.1. Faraday's Law; 2.2. Principle of Charge Conservation; Case One: The Stationary Field; Case Two: Quasi-Stationary Electromagnetic Field; 2.3. Distribution of Electric Charges; 2.3.1. Equation for the Volume Charge Density; 2.3.2. Uniform Medium
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|a 2.6. Equations for the Fields E and B2.7. Electromagnetic Potentials; 2.8. Maxwell's Equations for Sinusoidal Fields; 2.9. Electromagnetic Energy and Poynting Vector; 2.9.1. Principle of Energy Conservation and Joule's Law; 2.9.2. Energy Density and Poynting Vector; 2.9.3. Current Circuit and Transmission Line; 2.10. Uniqueness of the Forward Problem Solution; 2.10.1. Uniqueness Theorem; Case One; Case Two; 2.10.2. Formulation of the Boundary Value Problem; Reference; Further Reading; Chapter Three: Propagation of Electromagnetic Field in a Nonconducting Medium
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|a Example TwoExample Three; Example Four; Example Five; 1.3. Vector Potential of the Magnetic Field; 1.3.1. Relation Between Magnetic Field and Vector Potential; 1.3.2. Divergence and Laplacian of Vector Potential; 1.4. System of Equations of the Stationary Magnetic Field; 1.5. Examples of Magnetic Field of Current-Carrying Objects; 1.5.1. Example One: Magnetic Field of the Current Filament; 1.5.2. Example Two: The Vector Potential A and the Magnetic Field B of a Current in a Circular Loop; 1.5.3. Example Three: Magnetic Fields of the Magnetic Dipole; Some Comments
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|a Print version record
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| 650 |
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|a Induction logging
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| 650 |
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|a Induction logging
|2 fast
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| 700 |
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|a Itskovich, Gregory
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|i Print version:
|a Kaufman, Alex A
|t Basic Principles of Induction Logging : Electromagnetic Methods in Borehole Geophysics
|d Saint Louis : Elsevier Science, c2017
|z 9780128025833
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| 880 |
8 |
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|6 505-00/(S
|a 2.3.3. Nonuniform Medium2.3.4. Quasi-Stationary Field; 2.3.5. Behavior of Charge Density δ02; Example One; Example Two; 2.3.6. Surface Distribution of Charges; 2.3.7. Slowly Varying (Quasi-Stationary) Field; 2.4. Displacement Currents; 2.4.1. Second Source of the Magnetic Field; 2.4.2. Total Current and the Charge Conservation Principle; 2.4.3. Currents in the Circuit With a Capacitor; 2.5. Maxwell's Equations; 2.5.1. Introduction; 2.5.2. Maxwell's Equations; 2.5.3. Second Form of Maxwell's Equations; 2.5.4. Maxwell's Equations in a Piecewise Uniform Medium
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