Abstract:The alternating magnetic dynamo field of sea surface waves, a consequence of their Lorentz electric field, has been observed with a pair of simultaneously operated, closely spaced tri-axial magnetometers. Measurements from a magnetometer located in the centre of a tiny, uninhabited island served to compensate measurements from a near-shore magnetometer for magnetic pulsations of ionospheric origin, leaving the water wave dynamo field, effective close to shore only, as the dominant residual magnetic field. Ampl… Show more
“…The magnetic fields of ocean waves have been the subject of theoretical investigation by Longuet-Higgins et al (1954), Weaver (1965), Beal & Weaver (1970), Podney (1975), Chave (1984) and Weaver (1997). Maclure et al (1964) and Ochadlick (1989) report measurements in agreement with the theory of Weaver (1965) and observations of the magnetic signals of ocean waves are also reported by Fraser (1966) and Watermann & Magunia (1997). The topic is naturally closely associated with the electric signals of such waves, which are studied in papers such as Cox et al (1978) and .…”
S U M M A R YOcean swells have a magnetic signal, caused by the motional induction of sea water moving in the steady main magnetic field of Earth. To check the character of such signals at the sea surface, a magnetometer has been set free from a ship to float unrestricted on the surface of the ocean for periods of several days. The path of the floating magnetometer was tracked by satellite; this procedure enabled also the eventual recovery of the magnetometer by the ship.Superimposed upon a background of slow change of magnetic field, as the magnetometer drifted across different patterns of crustal magnetization, are high-frequency signals generated by the strong ocean swell present at the time. These wave-generated signals are typically up to 5 nT trough-to-peak, consistent with theory for their generation by ocean swells several metres trough-to-peak in height.The power spectra of the magnetic signals show a consistent peak at period 13 s, appropriate for the known characteristics of ocean swell in the area. The power spectra then exhibit a strong (−7 power) fall-off as period decreases below 13 s. This strong fall-off is consistent with oceanographic observations of the spectra of surface swell, combined with motional induction theory.
“…The magnetic fields of ocean waves have been the subject of theoretical investigation by Longuet-Higgins et al (1954), Weaver (1965), Beal & Weaver (1970), Podney (1975), Chave (1984) and Weaver (1997). Maclure et al (1964) and Ochadlick (1989) report measurements in agreement with the theory of Weaver (1965) and observations of the magnetic signals of ocean waves are also reported by Fraser (1966) and Watermann & Magunia (1997). The topic is naturally closely associated with the electric signals of such waves, which are studied in papers such as Cox et al (1978) and .…”
S U M M A R YOcean swells have a magnetic signal, caused by the motional induction of sea water moving in the steady main magnetic field of Earth. To check the character of such signals at the sea surface, a magnetometer has been set free from a ship to float unrestricted on the surface of the ocean for periods of several days. The path of the floating magnetometer was tracked by satellite; this procedure enabled also the eventual recovery of the magnetometer by the ship.Superimposed upon a background of slow change of magnetic field, as the magnetometer drifted across different patterns of crustal magnetization, are high-frequency signals generated by the strong ocean swell present at the time. These wave-generated signals are typically up to 5 nT trough-to-peak, consistent with theory for their generation by ocean swells several metres trough-to-peak in height.The power spectra of the magnetic signals show a consistent peak at period 13 s, appropriate for the known characteristics of ocean swell in the area. The power spectra then exhibit a strong (−7 power) fall-off as period decreases below 13 s. This strong fall-off is consistent with oceanographic observations of the spectra of surface swell, combined with motional induction theory.
“…Maclure et al (1964) and Ochadlick (1989) report measurements in agreement with the theory of Weaver (1965), and observations of the magnetic signals of ocean waves are also reported by Fraser (1966) and Watermann and Magunia (1997). In particular, Ochadlick (1989) reports aeromagnetic measurements over deep water.…”
Ocean swells have a magnetic signal, caused by the motional induction of seawater moving in the steady main magnetic field of Earth. These signals may be sensed by a low-flying aircraft, carrying out aeromagnetic measurements over the ocean. The apparent spatial wavelength that such signals will have, when observed data are plotted out for geological purposes, can vary greatly. It will depend particularly on the relative speeds and directions of travel of the observing aircraft and the ocean swells. The apparent wavelength of the ocean swell magnetic signal cannot be less than the actual ocean swell wavelength. Generally, it is greater, and it can range up to infinity in value. For observations over continental shelves, the situation is complicated by the dependence of the swell phase-velocity on water depth, by which the swell speed generally slows as land is approached.
“…In the 1950s, the electromagnetic field fluctuations resulting from the movement of seawater across Earth's magnetic field caught the attention of physical oceanographers. This sparked research that led to the development of the theory of electromagnetic fields caused by ocean currents and surface and internal ocean waves based on Maxwell's equations (Von Arx 1950;Longuet-Higgins et al 1954;Crews and Futterman 1962;Maclure et al 1964;Warburton and Caminiti 1964;Weaver 1965;Fraser 1966;Larsen 1973;Beal and Weaver 1970;Sanford 1971;Podney 1975;Ochadlick 1989;Watermann and Magunia 1997;Lilley et al 2004). Podney (1975) did an extensive theoretical summary of electromagnetic fields generated by surface and internal waves.…”
A magnetic signature is created by secondary magnetic field fluctuations caused by the phenomenon of seawater moving in Earth’s magnetic field. A laboratory experiment was conducted at the SUrge STructure Atmosphere INteraction (SUSTAIN) facility to measure the magnetic signature of surface waves using a differential method: a pair of magnetometers, separated horizontally by one-half wavelength, were placed at several locations on the outer tank walls. This technique significantly reduced the extraneous magnetic distortions that were detected simultaneously by both sensors and additionally doubled the magnetic signal of surface waves. Accelerometer measurements and local gradients were used to identify magnetic noise produced from tank vibrations. Wave parameters of 4 m long waves with a 0.56 Hz frequency and a 0.1-m amplitude were used in this experiment. Freshwater and saltwater experiments were completed to determine the magnetic difference generated by the difference in conductivity. Tests with an empty tank were conducted to identify the noise of the facility. When the magnetic signal was put through spectral analysis, it showed the primary peak at the wave frequency (0.56 Hz) and less pronounced higher frequency harmonics, which are caused by the non-linearity of shallow water surface waves. The magnetic noise induced by the wavemaker and related vibrations peaked around 0.3 Hz, which was removed using filtering techniques. These results indicate that the magnetic signature produced by surface waves was an order of magnitude larger than in traditional model predictions. The discrepancy may be due to the magnetic permeability difference between water and air that is not considered in the traditional model.
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