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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Page 227
We encounter numerous examples of boundary conditions in field theory. For
example, we have already seen that the tangential components of E(x) are
continuous across a boundary surface. Also, the normal component of D(x) is
continuous ...
We encounter numerous examples of boundary conditions in field theory. For
example, we have already seen that the tangential components of E(x) are
continuous across a boundary surface. Also, the normal component of D(x) is
continuous ...
Page 461
It is a simple exercise to verify that in component form (12.54) is the familiar
continuity equation, V J = -dp/dt. Two of the Maxwell equations relate fields and
sources — Gauss's law and the Ampere-Maxwell law. Gauss's law is a scalar
equation, ...
It is a simple exercise to verify that in component form (12.54) is the familiar
continuity equation, V J = -dp/dt. Two of the Maxwell equations relate fields and
sources — Gauss's law and the Ampere-Maxwell law. Gauss's law is a scalar
equation, ...
Page 550
The tangential component of E must be 0 on the boundary curve C. In particular,
the z component in (14.77) must be 0, so for TM modes f = 0 on C. (14.78) The
same condition implies that the other tangential component of E, and the normal
...
The tangential component of E must be 0 on the boundary curve C. In particular,
the z component in (14.77) must be 0, so for TM modes f = 0 on C. (14.78) The
same condition implies that the other tangential component of E, and the normal
...
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Contents
History and Perspective | 1 |
Vector Calculus | 9 |
Basic Principles of Electrostatics | 44 |
Copyright | |
14 other sections not shown
Common terms and phrases
Ampere's law angle approximation asymptotic atom axis Biot-Savart law bound charge boundary conditions calculate capacitance capacitor cavity Chapter charge density charge distribution charge q classical component conducting conductor consider constant coordinates cross section curl current density curves cylinder derive determine diamagnetic dielectric direction distance divergence electric and magnetic electric field electromagnetic waves electron electrostatic equal equipotential example Exercise ferromagnetic field energy FIGURE finite flux force frequency Gauss's Law incident induced infinite inside integral Laplace's equation linear loop Lorentz transformation magnetic field material Maxwell equations mode momentum motion oscillation parallel particle perpendicular physics plane wave plates plot point charge polarization position Poynting vector problem propagation radiation radius region result satisfy scalar shown in Fig shows solenoid solution sphere spherical static surface charge density surface current symmetry tensor theorem theory unit length vacuum vector function vector potential velocity volume wavelength wire xy plane
Bibliographic information
| Title | Electromagnetism |
| Authors | Gerald L. Pollack, Daniel R. Stump |
| Edition | illustrated, reprint |
| Publisher | Addison Wesley, 2002 |
| Original from | the University of California |
| Digitized | 23 Nov 2010 |
| ISBN | 0805385673, 9780805385670 |
| Length | 620 pages |
| Subjects | › › Science / Physics / General |
| Export Citation | BiBTeX EndNote RefMan |