WebSep 12, 2024 · A purely reactive load, including that presented by a capacitor or inductor, has Z L = j X where X is reactance. In particular, an inductor is represented by X > 0 and a capacitor is represented by X < 0. We find Γ = − Z 0 + j X + Z 0 + j X The numerator and denominator have the same magnitude, so Γ = 1. WebJan 29, 2014 · One of the least understood phenomena in electrical engineering is the idea that electric and magnetic fields appear to leave a radio transmitting antenna to form what we know as radio waves. Most books fall just short of explaining this process by making statements that fields snap or jump off the antenna as they expand.

Antenna-Theory.com - Field Regions

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REACTIVE POWER – Applied Industrial Electricity

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