Elements of Electromagnetics is a textbook written by Matthew N.O. Sadiku, a professor of electrical engineering at Prairie View A&M University. The book covers the fundamental concepts and principles of electromagnetics, such as electric fields, magnetic fields, Maxwell's equations, plane waves, transmission lines, waveguides, antennas, and radiation. The book also provides numerous examples, problems, and applications to help students master the subject.
The sixth edition of Elements of Electromagnetics was published in 2014 by Oxford University Press. It features updated and revised content, new end-of-chapter summaries, new design-a-problem exercises, and new MATLAB-based computer projects. The book also comes with an online resource center that includes a solutions manual, PowerPoint slides, video lectures, and interactive quizzes.
One of the highlights of the sixth edition is the inclusion of page 241, which contains a detailed derivation of the Poynting vector and the Poynting theorem. The Poynting vector represents the directional energy flux density of an electromagnetic field, while the Poynting theorem states that the rate of energy transfer across a closed surface is equal to the net power delivered by the sources inside the surface. These concepts are essential for understanding the energy aspects of electromagnetic waves and fields.
Elements of Electromagnetics 6th Edition by Sadiku is a well-written and comprehensive textbook that covers the core topics of electromagnetics in a clear and rigorous manner. It is suitable for undergraduate and graduate students who are interested in learning more about this fascinating branch of physics and engineering.
In this section, we will review some of the key concepts and formulas from page 241 of Elements of Electromagnetics 6th Edition by Sadiku. We will also provide some examples and applications to illustrate the use of the Poynting vector and the Poynting theorem.
The Poynting vector S is defined as the cross product of the electric field E and the magnetic field H:
S = E x H
The Poynting vector has the units of watts per square meter (W/m) and represents the directional energy flux density of an electromagnetic field. In other words, it tells us how much energy is flowing per unit area per unit time in a given direction.
For example, consider a plane wave propagating in free space with an electric field E = E0cos(kz - wt)ax and a magnetic field H = H0cos(kz - wt)ay, where E0, H0, k, and w are constants. The Poynting vector for this wave is given by:
S = E x H = E0H0cos(kz - wt)az
This means that the energy flux density of the wave is proportional to the square of the cosine function and points in the positive z-direction. The average value of the Poynting vector over one period is:
S = 1/2 E0H0az
This is also equal to 1/2 Z0E0az, where Z0 = 377 ohms is the characteristic impedance of free space.
The Poynting theorem is a generalization of the conservation of energy principle for electromagnetic fields. It states that the rate of energy transfer across a closed surface S is equal to the net power delivered by the sources inside S plus the rate of decrease of electromagnetic energy stored inside S. Mathematically, this can be expressed as:
dS . S = -dW/dt - integral dV . J . E
In this equation, dS . S is the outward flux of the Poynting vector over S, -dW/dt is the rate of decrease of electromagnetic energy density inside S, and dV . J . E is the net power delivered by the sources inside S.
The Poynting theorem can be used to calculate the power absorbed or radiated by various objects in electromagnetic fields. For example, consider a spherical shell with radius R and conductivity s that surrounds a point source with power P at its center. The electric field inside and outside the shell is given by:
Ei(r) = (P/4perr)-1/2ar, r <= R