Global atmospheric electrical circuit

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Lightning strikes the earth 100 times per second. Lightning strikes mountain top.jpg
Lightning strikes the earth 100 times per second.

A global atmospheric electrical circuit is the continuous movement of atmospheric charge carriers, such as ions, between an upper conductive layer (often an ionosphere) and surface. The global circuit concept is closely related to atmospheric electricity, but not all atmospheres necessarily have a global electric circuit. [2] The basic concept of a global circuit is that through the balance of thunderstorms and fair weather, the atmosphere is subject to a continual and substantial electrical current.

Contents

Principally, thunderstorms throughout the world carry negative charges to the earth, which is then discharged gradually through the air away from the storms, in conditions that are referred to as "fair weather". [1]

This atmospheric circuit is central to the study of atmospheric physics and meteorology. [3] The global electrical circuit is also relevant to the study of human health and air pollution, due to the interaction of ions and aerosols. The effects of climate change and temperature-sensitivity of the Earth's electrical circuit are currently unknown. [4]

History

The history of the global atmospheric electrical circuit is intertwined with the history of atmospheric electricity. For example, in the 18th century, scientists began understanding the link between lightning and electricity. In addition to the iconic kite experiments of Benjamin Franklin and Thomas-François Dalibard, some early studies of charge in a "cloudless atmosphere" (i.e. fair weather) were carried out by Giambatista Beccaria, John Canton, Louis-Guillaume Le Monnier and John Read. [5]

Fair weather measurements from the late 18th century onwards often found consistent diurnal variations. During the 19th century, several long series of observations were made. Measurements near cities were (and still are) heavily influenced by smoke pollution. In the early 20th century, balloon ascents provided information about the electric field well above the surface. Important work was done by the research vessel Carnegie , which produced standardised measurements around the world's oceans (where the air is relatively clean).

C. T. R. Wilson was the first to present the concept of a global circuit in 1920. [6]

Mechanism

Lightning

There are about 40,000 thunderstorms per day, generating roughly 100 lightning strikes per second, [1] which can be thought to charge the earth like a battery. Thunderstorms generate an electrical potential difference between the earth's surface and the ionosphere, mainly by means of lightning returning current to ground. Because of this, the ionosphere is positively charged relative to the earth. Consequently, there is always a small current of approximately 2pA per square metre transporting charged particles in the form of atmospheric ions between the ionosphere and the surface.

Fair weather

This current is carried by ions present in the atmosphere (generated mainly by cosmic rays in the free troposphere and above, and by radioactivity in the lowest 1km or so). The ions make the air weakly conductive; different locations, and meteorological conditions have different electrical conductivity. Fair weather describes the atmosphere away from thunderstorms where this weak electrical current between the ionosphere and the earth flows. [7]

Measurement

The voltages involved in the Earth's circuit are significant. At sea level, the typical potential gradient in fair weather is 120 V/m. Nonetheless, since the conductivity of air is limited, the associated currents are also limited. A typical value is 1800  A over the entire planet. When it is not rainy or stormy, the amount of electricity within the atmosphere[ clarification needed ] is typically between 1000 and 1800 amps. In fair weather, there are about 3.5 microamps per square kilometer (9 microamps per square mile). [8]

Carnegie curve

The Earth's electrical current varies according to a daily pattern called the Carnegie curve, caused by the regular daily variations in atmospheric electrification associated with the earth's stormy regions. [9] The pattern also shows seasonal variation, linked to the earth's solstices and equinoxes. It was named after the Carnegie Institution for Science.

See also

External sources

Publications

  • Le Monnier, L.-G.: "Observations sur l'Electricité de l'Air", Histoire de l'Académie royale des sciences (1752) , pp. 233ff. 1752.
  • Sven Israelsson, On the Conception Fair Weather Condition in Atmospheric Electricity. 1977.
  • Ogawa, T., "Fair-weather electricity". J. Geophys. Res., 90, 5951–5960, 1985.
  • Wåhlin, L., "Elements of fair weather electricity". J. Geophys. Res., 99, 10767-10772, 1994
  • RB Bent, WCA Hutchinson, Electric space charge measurements and the electrode effect within the height of a 21 m mast. J. Atmos. Terr. Phys, 196.
  • Bespalov P.A., Chugunov Yu. V. and Davydenko S.S., Planetary electric generator under fair-weather condition with altitude-dependent atmospheric conductivity, Journal of Atmospheric and Terrestrial Physics, v.58, #5,pp. 605–611,1996
  • DG Yerg, KR Johnson, Short-period fluctuations in the fair weather electric field. J. Geophys. Res., 1974.
  • T Ogawa, Diurnal variation in atmospheric electricity. J. Geomag. Geoelect, 1960.
  • R Reiter, Relationships Between Atmospheric Electric Phenomena and Simultaneous Meteorological Conditions. 1960
  • J. Law, The ionisation of the atmosphere near the ground in fair weather. Quarterly Journal of the Royal Meteorological Society, 1963
  • T. Marshall, W.D. Rust, M. Stolzenburg, W. Roeder, P. Krehbim A study of enhanced fair-weather electric fields occurring soon after sunrise.
  • R Markson, Modulation of the earth's electric field by cosmic radiation . Nature, 1981
  • Clark, John Fulmer, The Fair Weather Atmospheric Electric Potential and its Gradient.
  • P. A. Bespalov, Yu. V. Chugunov and S. S. Davydenko, Planetary electric generator under fair-weather conditions with altitude-dependent atmospheric conductivity.
  • AM Selva, et al., A New Mechanism for the Maintenance of Fair Weather Electric Field and Cloud Electrification.
  • M. J. Rycroft, S. Israelssonb and C. Pricec, The global atmospheric electric circuit, solar activity and climate change.
  • A. Mary Selvam, A. S. Ramachandra Murty, G. K. Manohar, S. S. Kandalgaonkar, Bh. V.Ramana Murty, A New Mechanism for the Maintenance of Fair Weather Electric Field and Cloud Electrification . arXiv:physics/9910006
  • Ogawa, Toshio, Fair-Weather electricity. Journal of Geophysical Research, Volume 90, Issue D4, pp. 5951–5960.
  • An auroral effect on the fair weather electric field. Nature 278, 239–241 (15 March 1979); doi:10.1038/278239a0
  • Bespalov, P. A.; Chugunov, Yu. V., Plasmasphere rotation and origin of atmospheric electricity. Physics – Doklady, Volume 39, Issue 8, August 1994, pp. 553–555
  • Bespalov, P. A.; Chugunov, Yu. V.; Davydenko, S. S. Planetary electric generator under fair-weather conditions with altitude-dependent atmospheric conductivity. Journal of Atmospheric and Terrestrial Physics.
  • A.J. Bennett, R.G. Harrison, A simple atmospheric electrical instrument for educational use

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<span class="mw-page-title-main">Thermosphere</span> Layer of the Earths atmosphere above the mesosphere and below the exosphere

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<span class="mw-page-title-main">Geophysics</span> Physics of the Earth and its vicinity

Geophysics is a subject of natural science concerned with the physical processes and physical properties of the Earth and its surrounding space environment, and the use of quantitative methods for their analysis. Geophysicists, who usually study geophysics, physics, or one of the Earth sciences at the graduate level, complete investigations across a wide range of scientific disciplines. The term geophysics classically refers to solid earth applications: Earth's shape; its gravitational, magnetic fields, and electromagnetic fields ; its internal structure and composition; its dynamics and their surface expression in plate tectonics, the generation of magmas, volcanism and rock formation. However, modern geophysics organizations and pure scientists use a broader definition that includes the water cycle including snow and ice; fluid dynamics of the oceans and the atmosphere; electricity and magnetism in the ionosphere and magnetosphere and solar-terrestrial physics; and analogous problems associated with the Moon and other planets.

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<span class="mw-page-title-main">Swarm (spacecraft)</span>

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<span class="mw-page-title-main">Outline of geophysics</span> Topics in the physics of the Earth and its vicinity

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The impact of the solar wind onto the magnetosphere generates an electric field within the inner magnetosphere - the convection field-. Its general direction is from dawn to dusk. The co-rotating thermal plasma within the inner magnetosphere drifts orthogonal to that field and to the geomagnetic field Bo. The generation process is not yet completely understood. One possibility is viscous interaction between solar wind and the boundary layer of the magnetosphere (magnetopause). Another process may be magnetic reconnection. Finally, a hydromagnetic dynamo process in the polar regions of the inner magnetosphere may be possible. Direct measurements via satellites have given a fairly good picture of the structure of that field. A number of models of that field exists.

Brian Tinsley is a physicist who for more than 60 years has been actively researching atmospheric and space physics. He has been a professor of physics at the University of Texas at Dallas since 1976 and has served many national and international scientific organizations. He obtained his PhD from the University of Canterbury in New Zealand in November, 1963, for research on optical emissions from the upper atmosphere. With his wife, Beatrice Tinsley, he came to Dallas to work at the newly formed Southwest Center for Advanced Studies, which became the University of Texas at Dallas in 1969. They divorced in 1978, their adopted children Alan and Theresa remaining with him.

In the height region between about 85 and 200 km altitude on Earth, the ionospheric plasma is electrically conducting. Atmospheric tidal winds due to differential solar heating or due to gravitational lunar forcing move the ionospheric plasma against the geomagnetic field lines thus generating electric fields and currents just like a dynamo coil moving against magnetic field lines. That region is therefore called ionospheric dynamo region. The magnetic manifestation of these electric currents on the ground can be observed during magnetospheric quiet conditions. They are called Sq-variations and L-variations (L=lunar) of the geomagnetic field. Additional electric currents are generated by the varying magnetospheric electric convection field. These are the DP1-currents and the polar DP2-currents. Finally, a polar-ring current has been derived from the observations which depends on the polarity of the interplanetary magnetic field. These geomagnetic variations belong to the so-called external part of the geomagnetic field. Their amplitudes reach at most about 1% of the main internal geomagnetic field Bo.

Giles Harrison is a Professor of Atmospheric Physics in the Department of Meteorology at the University of Reading, where he has served as Head of Department several times. He is a Visiting Professor at the Universities of Bath and Oxford. His research work continues over 250 years of UK studies in atmospheric electricity, in its modern form an interdisciplinary topic at the intersection of aerosol and cloud physics, solar-climate and internal-climate interactions, scientific sensor development and the retrieval of quantitative data from historical sources.

Michael John Rycroft is an ionospheric physicist.

Karen Aplin is a British atmospheric and space physicist. She is currently a professor at the University of Bristol. Aplin has made significant contributions to interdisciplinary aspects of space and terrestrial science, in particular the importance of electrical effects on planetary atmospheres. She was awarded the 2021 James Dungey Lectureship of the Royal Astronomical Society.

A Pedersen current is an electric current formed in the direction of the applied electric field when a conductive material with charge carriers is acted upon by an external electric field and an external magnetic field. Pedersen currents emerge in a material where the charge carriers collide with particles in the conductive material at approximately the same frequency as the gyratory frequency induced by the magnetic field. Pedersen currents are associated with a Pedersen conductivity related to the applied magnetic field and the properties of the material.

References

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  8. Mathew, Terry (2006). Elert, Glenn (ed.). "Electric current through the atmosphere". The Physics Factbook. Retrieved 25 January 2022.
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