Wilson effect

Last updated
Diagram of the Wilson effect. The umbra is the darker inner circle and the penumbra is the lighter ring around the umbra. Wilson effect.svg
Diagram of the Wilson effect. The umbra is the darker inner circle and the penumbra is the lighter ring around the umbra.

In astronomy, the Wilson effect is the perceived depression of a sunspot's umbra, or center, in the Sun's photosphere. The magnitude of the depression for the umbra is between 500 and 1000 km, with an average of 600 km. [1]

Contents

Sunspots result from the blockage of convective heat transport by intense magnetic fields. Sunspots are cooler than the rest of the photosphere, with effective temperatures of about 4,000°C (about 7,000°F). Sunspot occurrence follows an approximately 11-year period known as the solar cycle, discovered by Heinrich Schwabe in the 19th century.

History

Wilson's original sketch demonstrating the Wilson effect. Wilson effect original.jpg
Wilson's original sketch demonstrating the Wilson effect.

In 1769, during solar cycle 2, Scottish astronomer Alexander Wilson, working at the Macfarlane Observatory, noticed that the shape of sunspots noticeably flattened as they approached the Sun's limb due to solar rotation. [2] These observations were published in 1774 [3] and showed that sunspots were features on the solar surface, as opposed to minor planets or objects above it. Moreover, he observed what is now termed the Wilson effect: the penumbra and umbra vary in the manner expected by perspective effects if the umbrae of the spots are in fact slight depressions in the surface of the photosphere. [4]

Alternate interpretations

While the surface-depression interpretation of the Wilson effect is widespread, Bray and Loughhead contended that "the true explanation of the Wilson effect lies in the higher transparency of the spot material compared to the photosphere". [2] :93–99 A similar interpretation was expressed by C.H. Tong. [5]

See also

Related Research Articles

<span class="mw-page-title-main">Stellar corona</span> Outermost layer of a stars atmosphere

A corona is the outermost layer of a star's atmosphere. It consists of plasma.

<span class="mw-page-title-main">Sun</span> Star in the Solar System

The Sun is the star at the center of the Solar System. It is a massive, hot ball of plasma, inflated and heated by energy produced by nuclear fusion reactions at its core. Part of this internal energy is emitted from its surface as light, ultraviolet, and infrared radiation, providing most of the energy for life on Earth.

<span class="mw-page-title-main">Sunspot</span> Temporary phenomena on the Suns photosphere

Sunspots are phenomena on the Sun's photosphere that appear as temporary spots that are darker than the surrounding areas. They are regions of reduced surface temperature caused by concentrations of magnetic flux that inhibit convection. Sunspots appear within active regions, usually in pairs of opposite magnetic polarity. Their number varies according to the approximately 11-year solar cycle.

<span class="mw-page-title-main">Maunder Minimum</span> Period of low solar activity from 1645 to 1715

The Maunder Minimum, also known as the "prolonged sunspot minimum", was a period around 1645 to 1715 during which sunspots became exceedingly rare. During a 28-year period (1672–1699) within the minimum, observations revealed fewer than 50 sunspots. This contrasts with the typical 40,000–50,000 sunspots seen in modern times over a similar timespan.

<span class="mw-page-title-main">Photosphere</span> Stars outer shell from which light is radiated

The photosphere is a star's outer shell from which light is radiated. It extends into a star's surface until the plasma becomes opaque, equivalent to an optical depth of approximately 23, or equivalently, a depth from which 50% of light will escape without being scattered.

Starspots are stellar phenomena, so-named by analogy with sunspots. Spots as small as sunspots have not been detected on other stars, as they would cause undetectably small fluctuations in brightness. The commonly observed starspots are in general much larger than those on the Sun: up to about 30% of the stellar surface may be covered, corresponding to starspots 100 times larger than those on the Sun.

<span class="mw-page-title-main">Solar cycle</span> Periodic change in the Suns activity

The solar cycle, also known as the solar magnetic activity cycle, sunspot cycle, or Schwabe cycle, is a nearly periodic 11-year change in the Sun's activity measured in terms of variations in the number of observed sunspots on the Sun's surface. Over the period of a solar cycle, levels of solar radiation and ejection of solar material, the number and size of sunspots, solar flares, and coronal loops all exhibit a synchronized fluctuation from a period of minimum activity to a period of a maximum activity back to a period of minimum activity.

Richard Christopher Carrington was an English amateur astronomer whose 1859 astronomical observations demonstrated the existence of solar flares as well as suggesting their electrical influence upon the Earth and its aurorae; and whose 1863 records of sunspot observations revealed the differential rotation of the Sun.

<span class="mw-page-title-main">Spörer's law</span> Concept in astronomy

Spörer's law predicts the variation of sunspot latitudes during a solar cycle. It was discovered by the English astronomer Richard Christopher Carrington around 1861. Carrington's work was refined by the German astronomer Gustav Spörer.

<span class="mw-page-title-main">Georg Heinrich Thiessen</span> German astronomer

Georg Heinrich Thiessen was a German astronomer.

<span class="mw-page-title-main">Rudolf Wolf</span> Swiss astronomer and mathematician (1816–1893)

Johann Rudolf Wolf was a Swiss astronomer and mathematician best known for his research on sunspots.

The Evershed effect, named after the British astronomer John Evershed, is the radial flow of gas across the photospheric surface of the penumbra of sunspots from the inner border with the umbra towards the outer edge.

Solar physics is the branch of astrophysics that specializes in the study of the Sun. It deals with detailed measurements that are possible only for our closest star. It intersects with many disciplines of pure physics, astrophysics, and computer science, including fluid dynamics, plasma physics including magnetohydrodynamics, seismology, particle physics, atomic physics, nuclear physics, stellar evolution, space physics, spectroscopy, radiative transfer, applied optics, signal processing, computer vision, computational physics, stellar physics and solar astronomy.

<span class="mw-page-title-main">Alexander Wilson (astronomer)</span>

Alexander Wilson was a Scottish surgeon, type-founder, astronomer, mathematician and meteorologist. He was the first scientist to use kites in meteorological investigations.

The solar dynamo is a physical process that generates the Sun's magnetic field. It is explained with a variant of the dynamo theory. A naturally occurring electric generator in the Sun's interior produces electric currents and a magnetic field, following the laws of Ampère, Faraday and Ohm, as well as the laws of fluid dynamics, which together form the laws of magnetohydrodynamics. The detailed mechanism of the solar dynamo is not known and is the subject of current research.

<span class="mw-page-title-main">Coronal loop</span> Arch-like structure in the Suns corona

In solar physics, a coronal loop is a well-defined arch-like structure in the Sun's atmosphere made up of relatively dense plasma confined and isolated from the surrounding medium by magnetic flux tubes. Coronal loops begin and end at two footpoints on the photosphere and project into the transition region and lower corona. They typically form and dissipate over periods of seconds to days and may span anywhere from 1 to 1,000 megametres in length.

An active region is a temporary region in the Sun's atmosphere characterized by a strong and complex magnetic field. They are often associated with sunspots and are commonly the source of violent eruptions such as coronal mass ejections and solar flares. The number and location of active regions on the solar disk at any given time is dependent on the solar cycle.

<span class="mw-page-title-main">Solar cycle 2</span> Solar activity from June 1766 to June 1775

Solar cycle 2 was the second solar cycle since 1755, when extensive recording of sunspot activity began. The solar cycle lasted 9 years, beginning in June 1766 and ending in June 1775. The maximum smoothed sunspot number observed during the solar cycle was 193.0, and the starting minimum was 18.6.

Solar observation is the scientific endeavor of studying the Sun and its behavior and relation to the Earth and the remainder of the Solar System. Deliberate solar observation began thousands of years ago. That initial era of direct observation gave way to telescopes in the 1600s followed by satellites in the twentieth century.

<span class="mw-page-title-main">Solar phenomena</span> Natural phenomena within the Suns atmosphere

Solar phenomena are natural phenomena which occur within the atmosphere of the Sun. These phenomena take many forms, including solar wind, radio wave flux, solar flares, coronal mass ejections, coronal heating and sunspots.

References

  1. Löptien, B.; Lagg, A.; van Noort, M.; Solanki, S. K. (Nov 2018). "Measuring the Wilson depression of sunspots using the divergence-free condition of the magnetic field vector". Astronomy & Astrophysics. 619: A42. arXiv: 1808.06867 . doi:10.1051/0004-6361/201833571.
  2. 1 2 R.J. Bray and R.E. Loughhead (1965) Sunspots, page 4 "Discovery of the Wilson Effect", John Wiley & Sons
  3. Wilson, A.; Maskelyne, N. (1774). "Observations on the Solar Spots. By Alexander Wilson, M. D. Professor of Practical Astronomy in the University of Glasgow. Communicated by the Rev. Nevil Maskelyne, Astronomer Royal". Philosophical Transactions (1683-1775). 64: 1–30.
  4. John H. Thomas and Nigel O. Weiss (1991) Sunspots:Theory and Observations, page 5: "Wilson depression", Kluwer Academic Publishers
  5. C.H. Tong (2005) "Imaging sunspots using helioseismic methods", Philosophical Transactions of the Royal Society A 363:276175