Empirical Earth · Radio & Long-Distance Signals
Radio propagation — why distance needs bending
The claim
“Radio travels in straight lines, so a signal crossing an ocean proves there’s no curve.”
What is measured
AM and shortwave signals reach past the horizon by bouncing off the ionosphere ~100–300 km up. The curve is the reason they need the bounce. See the band-by-band radio distance records and the radio band plan.
What would show this is wrong
over-horizon signals that required no ionospheric refraction around a curved Earth to explain.
Sources
- ITU-R Recommendation P.453. The radio refractive index: its formula and refractivity data (water-vapor term, N-units). International Telecommunication Union. ITU-R P.453 link
- HF ground-wave & skywave propagation. ARRL Antenna Book & Handbook; ITU-R P.368 (ground wave) and P.533 (HF skywave prediction). skywave propagation link
- The ionosphere. D/E/F-layer structure and diurnal HF absorption; NOAA Space Weather Prediction Center; ITU-R P.531. ionosphere link
- Tropospheric ducting & Sporadic E. ITU-R P.834 (refraction); ARRL VHF/UHF propagation references — super-refraction ducting and Es VHF reflection. sporadic E link
- Marconi's transatlantic transmission (1901) & the Kennelly–Heaviside layer. Marconi, Poldhu → Signal Hill; A. E. Kennelly & O. Heaviside (1902); E. Appleton's confirmation (1920s, Nobel 1947 link
- LoRa / LoRaWAN & distance records. Semtech LoRa CSS modulation; The Things Network world records (766 km, 832 km @ 25 mW via high-altitude balloon; ≈1,336 km reported). thethingsnetwork.org link
- Fresnel zones in radio path design. Standard RF link engineering — first Fresnel-zone radius and ~60% clearance over earth-curvature (4/3) profiles (ITU-R P.526; microwave path-budget texts) link
- Marconi’s 1901 transatlantic “S” — method and the lasting dispute. A high-power spark-gap transmitter at Poldhu fed a kite-lofted wire, received on an untuned coherer and earphone; the Morse link
The full entry, with the working →