By Robert Paknys

ISBN-10: 1118940547

ISBN-13: 9781118940549

ISBN-10: 1118940555

ISBN-13: 9781118940556

ISBN-10: 1119127440

ISBN-13: 9781119127444

Knowing electromagnetic wave idea is pivotal within the layout of antennas, microwave circuits, radars, and imaging platforms. Researchers at the back of know-how advances in those and different components have to comprehend either the classical concept of electromagnetics in addition to sleek and rising ideas of fixing Maxwell's equations. To this finish, the e-book offers a graduate-level therapy of chosen analytical andRead more...

summary: realizing electromagnetic wave conception is pivotal within the layout of antennas, microwave circuits, radars, and imaging structures. Researchers at the back of know-how advances in those and different components have to comprehend either the classical thought of electromagnetics in addition to glossy and rising strategies of fixing Maxwell's equations. To this finish, the e-book presents a graduate-level remedy of chosen analytical and computational tools. The analytical equipment comprise the separation of variables, perturbation conception, Green's capabilities, geometrical optics, the geometrical thought of diffraction, actual optics, and the actual conception of diffraction. The numerical strategies contain mode matching, the tactic of moments, and the finite aspect approach. The analytical equipment supply actual insights which are precious within the layout technique and the discovery of recent units. The numerical equipment are extra in a position to treating common and complicated buildings. jointly, they shape a foundation for contemporary electromagnetic layout. the extent of presentation permits the reader to right away start utilising the tips on how to a few difficulties of reasonable complexity. It additionally presents reasons of the underlying theories in order that their functions and barriers should be understood

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**Extra resources for Applied frequency-domain electromagnetics**

**Example text**

This can be found by considering a point where ωt − kz = const. Then, the velocity is u = dz/dt = ω/k. √ √ Since k = ω μ , it follows that u = 1/ μ . Also, u = λf so that k = 2π/λ. 998 × 108 m/s, the speed of light. 7) becomes ∂2E x 1 ∂2E x − 2 =0 2 ∂z u ∂t2 √ where u = 1/ μ . The time-domain wave equation solution is not limited to cos(ωt ∓ kz). By substitution into the wave equation, it can be confirmed that Ex = K1 f (t − z/u) + K2 g(t + z/u) is a solution, where f and g are any twice-differentiable functions.

10 A magnetic field phasor is given by H = 12ˆ x sin ay A/m, where a is a constant. (a) Use ∇ × H to find E. Assume a non-conducting medium that has J = σE = 0. (b) From ∇ × E, find H. Under what condition does this equal the original H that we started with? 76, find the frequency in MHz. 11 A current density phasor is J = x ˆJ0 e−ax A/m2 where J0 and a are constants. (a) Find the charge density phasor ρv . (b) Find the time-domain current J (t) and charge density v (t). 12 Free charges placed inside a conductor will repel each other, and as they move apart, the charge density will decay exponentially.

Show that the normal volume current Jz is continuous at z = 0. 17 An electric field in free space is given by E = x ˆE0 cos(ωt − kz) and J = σE = 0. (a) Take the curl of E and then integrate with respect to time, to get H. The constant of integration represents a magnetostatic solution; we can make it zero. (b) Now take the curl of H and integrate with respect to time to get E. (c) What is the required relationship between ω and k so that after the two curl operations, we get back the original E?

### Applied frequency-domain electromagnetics by Robert Paknys

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