By Jack Vanderlinde

ISBN-10: 9048167078

ISBN-13: 9789048167074

This e-book is a self contained path in electromagnetic conception appropriate for senior physics and electric engineering scholars in addition to graduate scholars whose prior has now not ready them good for books resembling Jackson or Landau and Lifschitz. The textual content is liberally sprinkled with labored examples illustrating the appliance of the speculation to numerous actual problems. This new edition features improved accuracy and clarity, further and extra clarified examples, plus extra sections on Schwarz-Christoffel mappings. Making the booklet extra self sufficient, an appendix on orthogonal functionality expansions and the derivation of Bessel features and Legendre polynomials in addition to derivation in their producing services are each one integrated. The quantity of exercises has additionally been elevated by way of forty five over the former edition.

This publication stresses the harmony of electromagnetic idea with electrical and magnetic fields built in parallel. SI devices are used all through and enormous use is made up of tensor notation and the Levi-Cevita image. To extra heavily demonstrate the parallelism, huge use is made up of the scalar magnetic strength relatively in facing the Laplace and Poisson equation. eighty five labored difficulties illustrate the speculation. Conformal mappings are handled in a few aspect. proper mathematical fabric is supplied in appendices.

For information about recommendations handbook, please touch the writer Jack Vanderlinde at: jvd@unb.ca or see "Related hyperlinks - resolution Manual".

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**Additional resources for Classical Electromagnetic Theory**

**Example text**

As we will see when discussing the covariant formulation in Chapter 11, the potentials V and A appear to be somewhat more fundamental than E and B in the relativistic formulation as well. It is worth noting that according to (1–52), A is always parallel to the mean weighted current ﬂow. We note also that from its deﬁnition, A is not unique. We can add the gradient of any function, say Λ(r ), to A without changing curl A. 5 See for example R. P. Feynman, R. B. Leighton, and M. Sands (1964) The Feynman Lectures on Physics, Vol.

Speciﬁcally, −J(r ) × ∇ 1 r−r =∇× J(r ) r−r − 1 ∇ × J(r ) r−r (1–41) Because ∇ acts only on the unprimed coordinates, the term ∇ × J(r ) vanishes and because the integral is over the primed coordinates, we can take the curl outside the integral to yield J(r ) 3 µ0 ∇× (1–42) B(r ) = d r 4π r−r As the divergence of any curl vanishes (11) we note in passing that ∇ · B(r ) = 0, (1–43) an important result that is the analogy of Gauss’ law for Electric ﬁelds. Equation (1– 43) implies via Gauss’ theorem that no isolated magnetic monopoles exist because no volume can be found such that the integrated magnetic charge density is nonzero.

Feynman, R. B. Leighton, and M. Sands (1964) The Feynman Lectures on Physics, Vol. ). 13: Find the vector potential A(0, 0, z) above a circular current loop of radius a in the x-y plane. Solution: J = I δ(r −a) δ(z ) ϕˆ where r is the radial coordinate of a current element in cylindrical coordinates. 3) Since we expect B to have no x or y component at this point, A should not have any z dependence. Clearly this result is not very useful. We will tackle this problem again using the magnetic scalar potential.

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