ElectromagnetismElectromagnetism sets a new standard in physics education. Throughout the book, the theory is illustrated with real-life applications in modern technology. It also includes detailed work examples and step-by-step explanations to help readers develop their problem-solving strategies and skills and consolidate their understanding. In addition to a meticulous development of thse traditional, analytical mathematical approaches, readers are also introduced to a range of techniques required for solving problems using computers. Electromagnetism provides an ideal preparation for readers who plan advanced studies in electrodynamics as well as those moving into industry or engineering . |
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... equal to the area of the parallelogram defined by A and B. ( b ) Why is the equation A × B = AB sin @ false ? ( c ) Prove that A · ( B × C ) is equal to the determinant Ax Ay Az Bx By B2 Cx Cy Cz ( d ) Show that A · ( B × C ) is equal ...
... equal but opposite , the contributions of the outer two surfaces must also be equal but opposite to have E = 0 , which requires Q1 Q2u . Qu = The solution to the four equations is Q11 = Q2u = ( Q ' + Q ′′ ) / 2 Q1u = -Q21 = ( Q ' — Q ...
... equal to -dQ / dt , where Q is the charge enclosed by Σ . To derive the boundary condition , let h → 0 . In the limit , the cylindrical side of Σ approaches 0 in area , so the flux through it approaches 0 ; and the top and bottom faces ...
Contents
History and Perspective | 1 |
Vector Calculus | 9 |
Basic Principles of Electrostatics | 44 |
Copyright | |
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