Entries by rude man

Es vs Em Fields in Electrodynamics: Capacitor & Antenna

Abstract The analysis of the two kinds of electric fields, namely the irrotational and non-conservative, is extended to electrodynamics, as exemplified by the high-frequency behavior of a parallel-plate capacitor and a radiating antenna. Since the concept of split electric fields still seems unfamiliar in some quarters, I will start back at square one by quoting…

Electric Vector Potential: Detect Non-Conservative Fields

Main Point The electric vector potential offers a means of determining the non-conservative component of a mixed stationary or quasi-stationary electric field. Background: magnetic vector potential Many readers will be familiar with the static magnetic vector potential ## \bf A = (\mu/4\pi) \int \bf j~ dv/s ## with ## \bf j ## = current (area)…

How to Recognize Split Electric Fields

Introduction In a previous Insight, A New Interpretation of Dr. Walter Lewin’s Paradox, I introduced the fact that there are two kinds of E fields.  One (Em) is generated whenever a source of emf is produced.  The other (Es) is the electrostatic field.  The Es field always terminates on free charges; the Em does not. …

Mixing vs Beating: Superheterodyne & Beat Frequency

Mixing vs. Beating: a brief history A long time ago I read a paper in the IEEE Proceedings recounting the history of the superheterodyne receiver. Overall it was a very interesting and informative article, with one exception: the author remarked that the modulation (or mixing) principle was nothing new and is already known to piano…

Brachistochrone Subway Tunnel: Fastest Tunnel Shape Explained

Introduction A subway tunnel could, in principle, operate without external energy (like electricity) if we assume zero friction everywhere. The train would descend, convert potential energy to kinetic energy, coast through a low point, then climb back up—all by exchanging potential and kinetic energy. Historical background What is the tunnel shape that minimizes travel time…

Mutual Inductance: When k≠1 and Two Coupling Coefficients

Mutual inductance and the coupling coefficient A commonly used formula for mutual inductance M between two nearby coils L1 and L2 is M = k√(L1*L2). This formula, however, assumes equal percentage flux linkages between the two coils. That requirement is often omitted in several references. Example: single-turn coil inside a long solenoid (Fig. 1) This…