Solar Activity Information
Solar variation is the change in the amount of radiation emitted by the Sun and in its spectral distribution over years to millennia. These variations have periodic components, the main one being the approximately 11-year solar cycle (or sunspot cycle). The changes also have aperiodic fluctuations.[1] In recent decades, solar activity has been measured by satellites, while before it was estimated using 'proxy' variables. Scientists studying climate change are interested in understanding the effects of variations in the total and spectral solar irradiance on Earth and its climate.
Variations in total solar irradiance were too small to detect with technology available before the satellite era, although the small fraction in ultra-violet light varies by a few percent. Total solar output is now measured to vary (over the last three 11-year sunspot cycles) by approximately 0.1%[2][3][4] or about 1.3 Watts per square meter (W/m2) peak-to-trough during the 11-year sunspot cycle. The amount of solar radiation received at the outer surface of Earth's atmosphere averages 1366 W/m2.[5][6][7] There are no direct measurements of the longer-term variation, and interpretations of proxy measures of variations differ. The intensity of solar radiation reaching Earth has been relatively constant through the last 2000 years, with variations of around 0.1-0.2%.[8][9][10] Solar variation, together with volcanic activity probably contributed to climate change, for example during the Maunder Minimum. However, changes in solar brightness are too weak to explain recent climate change.[11]
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History of study into solar variations
400 year history of sunspot numbers.The longest recorded aspect of solar variations are changes in sunspots. The first record of sunspots dates to around 800 BC in China and the oldest surviving drawing of a sunspot dates to 1128. In 1610, astronomers began using the telescope to make observations of sunspots and their motions. Initial study was focused on their nature and behavior.[12] Although the physical aspects of sunspots were not identified until the 20th century, observations continued. Study was hampered during the 17th century due to the low number of sunspots during what is now recognized as an extended period of low solar activity, known as the Maunder Minimum. By the 19th century, there was a long enough record of sunspot numbers to infer periodic cycles in sunspot activity. In 1845, Princeton University professors Joseph Henry and Stephen Alexander observed the Sun with a thermopile and determined that sunspots emitted less radiation than surrounding areas of the Sun. The emission of higher than average amounts of radiation later were observed from the solar faculae.[13]
Around 1900, researchers began to explore connections between solar variations and weather on Earth. Of particular note is the work of Charles Greeley Abbot. Abbot was assigned by the Smithsonian Astrophysical Observatory (SAO) to detect changes in the radiation of the Sun. His team had to begin by inventing instruments to measure solar radiation. Later, when Abbot was head of the SAO, it established a solar station at Calama, Chile to complement its data from Mount Wilson Observatory. He detected 27 harmonic periods within the 273-month Hale cycles, including 7, 13, and 39 month patterns. He looked for connections to weather by means such as matching opposing solar trends during a month to opposing temperature and precipitation trends in cities. With the advent of dendrochronology, scientists such as Waldo S. Glock attempted to connect variation in tree growth to periodic solar variations in the extant record and infer long-term secular variability in the solar constant from similar variations in millennial-scale chronologies.[14]
Statistical studies that correlate weather and climate with solar activity have been popular for centuries, dating back at least to 1801, when William Herschel noted an apparent connection between wheat prices and sunspot records.[15] They now often involve high-density global datasets compiled from surface networks and weather satellite observations and/or the forcing of climate models with synthetic or observed solar variability to investigate the detailed processes by which the effects of solar variations propagate through the Earth's climate system.[16]
Solar activity and irradiance measurement
Direct irradiance measurements have only been available during the last three cycles and are based on a composite of many different observing satellites.[17][18] However, the correlation between irradiance measurements and other proxies of solar activity make it reasonable to estimate past solar activity. Most important among these proxies is the record of sunspot observations that has been recorded since ~1610. Since sunspots and associated faculae are directly responsible for small changes in the brightness of the sun, they are closely correlated to changes in solar output. Direct measurements of radio emissions from the Sun at 10.7 cm also provide a proxy of solar activity that can be measured from the ground since the Earth's atmosphere is transparent at this wavelength. Lastly, solar flares are a type of solar activity that can impact human life on Earth by affecting electrical systems, especially satellites. Flares usually occur in the presence of sunspots, and hence the two are correlated, but flares themselves make only tiny perturbations of the solar luminosity.
Recently, it has been claimed that the total solar irradiance is varying in ways that are not duplicated by changes in sunspot observations or radio emissions. However, this conclusion is disputed. Some[who?] believe that shifts in irradiance may be the result of calibration problems in the measuring satellites.[19][20] These speculations also admit the possibility that a small long-term trend might exist in solar irradiance.[21]
Sunspots
Graph showing proxies of solar activity, including changes in sunspot number and cosmogenic isotope production.Sunspots are relatively dark areas on the radiating 'surface' (photosphere) of the Sun where intense magnetic activity inhibits convection and cools the photosphere. Faculae are slightly brighter areas that form around sunspot groups as the flow of energy to the photosphere is re-established and both the normal flow and the sunspot-blocked energy elevate the radiating 'surface' temperature. Scientists have speculated on possible relationships between sunspots and solar luminosity since the historical sunspot area record began in the 17th century.[22][23] Correlations are now known to exist with decreases in luminosity caused by sunspots (generally < - 0.3 %) and increases (generally < + 0.05 %) caused both by faculae that are associated with active regions as well as the magnetically active 'bright network'.[24] Modulation of the solar luminosity by magnetically active regions was confirmed by satellite measurements of total solar irradiance (TSI) by the ACRIM1 experiment on the Solar Maximum Mission (launched in 1980).[24] The modulations were later confirmed in the results of the ERB experiment launched on the Nimbus 7 satellite in 1978.[25] Sunspots in magnetically active regions are cooler and 'darker' than the average photosphere and cause temporary decreases in TSI of as much as 0.3 %. Faculae in magnetically active regions are hotter and 'brighter' than the average photosphere and cause temporary increases in TSI. The net effect during periods of enhanced solar magnetic activity is increased radiant output of the sun because faculae are larger and persist longer than sunspots.
There had been some suggestion that variations in the solar diameter might cause variations in output. But recent work, mostly from the Michelson Doppler Imager instrument on SOHO, shows these changes to be small, about 0.001% (Dziembowski et al., 2001).
Various studies have been made using sunspot number (for which records extend over hundreds of years) as a proxy for solar output (for which good records only extend for a few decades). Also, ground instruments have been calibrated by comparison with high-altitude and orbital instruments. Researchers have combined present readings and factors to adjust historical data. Other proxy data — such as the abundance of cosmogenic isotopes — have been used to infer solar magnetic activity and thus likely brightness.
Sunspot activity has been measured using the Wolf number for about 300 years. This index (also known as the Zürich number) uses both the number of sunspots and the number of groups of sunspots to compensate for variations in measurement. A 2003 study by Ilya Usoskin of the University of Oulu, Finland found that sunspots had been more frequent since the 1940s than in the previous 1150 years.[26]
Reconstruction of solar activity over 11,400 years. Period of equally high activity over 8,000 years ago marked.Sunspot numbers over the past 11,400 years have been reconstructed using dendrochronologically dated radiocarbon concentrations. The level of solar activity during the past 70 years is exceptional — the last period of similar magnitude occurred over 8,000 years ago. The Sun was at a similarly high level of magnetic activity for only ~10% of the past 11,400 years, and almost all of the earlier high-activity periods were shorter than the present episode.[27]
Solar activity events recorded in radiocarbon. Present period is on left. Values since 1900 not shown.| Event | Start | End |
|---|---|---|
| Oort minimum (see Medieval Warm Period) | 1040 | 1080 |
| Medieval maximum (see Medieval Warm Period) | 1100 | 1250 |
| Wolf minimum | 1280 | 1350 |
| Spörer Minimum | 1450 | 1550 |
| Maunder Minimum | 1645 | 1715 |
| Dalton Minimum | 1790 | 1820 |
| Modern Maximum | 1900 | present |
A list of historical Grand minima of solar activity [28] includes also Grand minima ca. 690 AD, 360 BC, 770 BC, 1390 BC, 2860 BC, 3340 BC, 3500 BC, 3630 BC, 3940 BC, 4230 BC, 4330 BC, 5260 BC, 5460 BC, 5620 BC, 5710 BC, 5990 BC, 6220 BC, 6400 BC, 7040 BC, 7310 BC, 7520 BC, 8220 BC, 9170 BC.
Solar cycles
Solar cycles are cyclic changes in behavior of the Sun. Many possible patterns have been suggested; only the 11 and 22 year cycles are clear in the observations.
2,300 year Hallstatt solar variation cycles.- 11 years: Most obvious is a gradual increase and more rapid decrease of the number of sunspots over a period ranging from 9 to 12 years, called the Schwabe cycle, named after Heinrich Schwabe. Differential rotation of the sun's convection zone (as a function of latitude) consolidates magnetic flux tubes, increases their magnetic field strength and makes them buoyant (see Babcock Model). As they rise through the solar atmosphere they partially block the convective flow of energy, cooling their region of the photosphere, causing 'sunspots'. The Sun's apparent surface, the photosphere, radiates more actively when there are more sunspots. Satellite monitoring of solar luminosity since 1980 has shown there is a direct relationship between the solar activity (sunspot) cycle and luminosity with a solar cycle peak-to-peak amplitude of about 0.1 %.[2] Luminosity has also been found to decrease by as much as 0.3 % on a 10 day timescale when large groups of sunspots rotate across the Earth's view and increase by as much as 0.05 % for up to 6 months due to faculae associated with the large sunspot groups.[24]
- 22 years: Hale cycle, named after George Ellery Hale. The magnetic field of the Sun reverses during each Schwabe cycle, so the magnetic poles return to the same state after two reversals.
- 87 years (70–100 years): Gleissberg cycle, named after Wolfgang Gleißberg, is thought to be an amplitude modulation of the 11-year Schwabe Cycle (Sonnett and Finney, 1990),[29] Braun, et al., (2005).[30]
- 210 years: Suess cycle (a.k.a. de Vries cycle). Braun, et al., (2005).[30]
- 2,300 years: Hallstatt cycle[31][32]
- 6000 years (Xapsos and Burke, 2009).[33]
Other patterns have been detected:
- In carbon-14: 105, 131, 232, 385, 504, 805, 2,241 years (Damon and Sonnett, 1991).
- During the Upper Permian 240 million years ago, mineral layers created in the Castile Formation show cycles of 2,500 years.
The sensitivity of climate to cyclical variations in solar forcing will be higher for longer cycles due to the thermal inertia of the ocean, which acts to damp high frequencies. Using a phenomenological approach, Scafetta and West (2005) found that the climate was 1.5 times as sensitive to 22 year cyclical forcing relative to 11 year cyclical forcing, and that the thermal inertial induced a lag of approximately 2.2 years in cyclic climate response in the temperature data.[34]
Predictions based on patterns
- A simple model based on emulating harmonics by multiplying the basic 11-year cycle by powers of 2 produced results similar to Holocene behavior. Extrapolation suggests a gradual cooling during the next few centuries with intermittent minor warmups and a return to near Little Ice Age conditions within the next 500 years. This cool period then may be followed approximately 1,500 years from now by a return to altithermal conditions similar to the previous Holocene Maximum.[35]
- There is weak evidence for a quasi-periodic variation in the sunspot cycle amplitudes with a period of about 90 years (Gleisberg cycle). These characteristics indicate that the next solar cycle should have a maximum smoothed sunspot number of about 145±30 in 2010 while the following cycle should have a maximum of about 70±30 in 2023.[36]
- Because carbon-14 cycles are quasi periodic, Damon and Sonett (1989) predict future climate:[37]
Solar irradiance, or insolation, is the amount of sunlight which reaches the Earth. The equipment used might measure optical brightness, total radiation, or radiation in various frequencies. Historical estimates use various measurements and proxies.
| Cycle length | Cycle name | Last positive carbon-14 anomaly | Next "warming" |
|---|---|---|---|
| 232 | --?-- | AD 1922 (cool) | AD 2038 |
| 208 | Suess | AD 1898 (cool) | AD 2210 |
| 88 | Gleisberg | AD 1986 (cool) | AD 2030 |
Solar irradiance of Earth and its surface
There are two common meanings:
- the radiation reaching the upper atmosphere
- the radiation reaching some point within the atmosphere, including the surface.
Various gases within the atmosphere absorb some solar radiation at different wavelengths, and clouds and dust also affect it. Measurements above the atmosphere are needed to determine variations in solar output, to avoid the confounding effects of changes within the atmosphere. There is some evidence that sunshine at the Earth's surface has been decreasing in the last 50 years (see global dimming) possibly caused by increased atmospheric pollution, whilst over roughly the same timespan solar output has been nearly constant.
Milankovitch cycle variations
Some variations in insolation are not due to solar changes but rather due to the Earth moving closer or further from the Sun, or changes in the latitudinal distribution of radiation. These have caused variations of as much as 25% (locally; global average changes are much smaller) in solar insolation over long periods. The most recent significant event was an axial tilt of 24° during boreal summer at near the time of the Holocene climatic optimum.
Further information: Milankovitch cyclesSolar interactions with Earth
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There are several hypotheses for how solar variations may affect Earth. Some variations, such as changes in the size of the Sun, are presently only of interest in the field of astronomy.
Changes in total irradiance
- Total solar irradiance changes slowly on decadal and longer timescales.
- The variation during recent solar magnetic activity cycles has been about 0.1% (peak-to-peak).[2]
- Variations corresponding to solar changes with periods of 9–13, 18–25, and >100 years have been detected in sea-surface temperatures.
- In contrast to older reconstructions,[38] most recent reconstructions of total solar irradiance point to an only small increase of only about 0.05 % to 0.1 % between Maunder Minimum and the present.[39][40][41]
- Different composite reconstructions of total solar irradiance observations by satellites show different trends since 1980; see the global warming section below.
Changes in ultraviolet irradiance
- Ultraviolet irradiance (EUV) varies by approximately 1.5 percent from solar maxima to minima, for 200 to 300 nm UV.[42]
- Energy changes in the UV wavelengths involved in production and loss of ozone have atmospheric effects.
- The 30 hPa atmospheric pressure level has changed height in phase with solar activity during the last 4 solar cycles.
- UV irradiance increase causes higher ozone production, leading to stratospheric heating and to poleward displacements in the stratospheric and tropospheric wind systems.
- A proxy study estimates that UV has increased by 3% since the Maunder Minimum.[citation needed]
Changes in the solar wind and the Sun's magnetic flux
- A more active solar wind and stronger magnetic field reduces the cosmic rays striking the Earth's atmosphere.
- Variations in the solar wind affect the size and intensity of the heliosphere, the volume larger than the Solar System filled with solar wind particles.
- Cosmogenic production of 14C, 10Be and 36Cl show changes tied to solar activity.
- Cosmic ray ionization in the upper atmosphere does change, but significant effects are not obvious.
- As the solar coronal-source magnetic flux doubled during the past century, the cosmic-ray flux has decreased by about 15%.
- The Sun's total magnetic flux rose by a factor of 1.41 from 1964–1996 and by a factor of 2.3 since 1901.
Effects on clouds
- Cosmic rays have been hypothesized to affect formation of clouds through possible effects on production of cloud condensation nuclei. Observational evidence for such a relationship is inconclusive.
- 1983–1994 data from the International Satellite Cloud Climatology Project (ISCCP) showed that global low cloud formation was highly correlated with cosmic ray flux; subsequent to this the correlation breaks down.[43]
Other effects due to solar variation
Interaction of solar particles, the solar magnetic field, and the Earth's magnetic field, cause variations in the particle and electromagnetic fields at the surface of the planet. Extreme solar events can affect electrical devices. Weakening of the Sun's magnetic field is believed to increase the number of interstellar cosmic rays which reach Earth's atmosphere, altering the types of particles reaching the surface. It has been speculated that a change in cosmic rays could cause an increase in certain types of clouds, affecting Earth's albedo.
Geomagnetic effects
Solar particles interact with Earth's magnetosphereThe Earth's polar aurorae are visual displays created by interactions between the solar wind, the solar magnetosphere, the Earth's magnetic field, and the Earth's atmosphere. Variations in any of these affect aurora displays.
Sudden changes can cause the intense disturbances in the Earth's magnetic fields which are called geomagnetic storms.
Solar proton events
Energetic protons can reach Earth within 30 minutes of a major flare's peak. During such a solar proton event, Earth is showered in energetic solar particles (primarily protons) released from the flare site. Some of these particles spiral down Earth's magnetic field lines, penetrating the upper layers of our atmosphere where they produce additional ionization and may produce a significant increase in the radiation environment.
Galactic cosmic rays
Solar wind and magnetic field create heliosphere around solar system.An increase in solar activity (more sunspots) is accompanied by an increase in the "solar wind," which is an outflow of ionized particles, mostly protons and electrons, from the sun. The Earth's geomagnetic field, the solar wind, and the solar magnetic field deflect galactic cosmic rays (GCR). A decrease in solar activity increases the GCR penetration of the troposphere and stratosphere. GCR particles are the primary source of ionization in the troposphere above 1 km (below 1 km, radon is a dominant source of ionization in many areas).
Levels of GCRs have been indirectly recorded by their influence on the production of carbon-14 and beryllium-10. The Hallstatt solar cycle length of approximately 2300 years is reflected by climatic Dansgaard-Oeschger events. The 80–90 year solar Gleissberg cycles appear to vary in length depending upon the lengths of the concurrent 11 year solar cycles, and there also appear to be similar climate patterns occurring on this time scale.
Cloud effects
Changes in ionization affect the abundance of aerosols that serve as the nuclei of condensation for cloud formation.[44] As a result, ionization levels potentially affect levels of condensation, low clouds, relative humidity, and albedo due to clouds. Clouds formed from greater amounts of condensation nuclei are brighter, longer lived, and likely to produce less precipitation. Changes of 3–4% in cloudiness and concurrent changes in cloud top temperatures have been correlated to the 11 and 22 year solar (sunspot) cycles, with increased GCR levels during "antiparallel" cycles.[45] Global average cloud cover change has been found to be 1.5–2%. Several studies of GCR and cloud cover variations have found positive correlation at latitudes greater than 50° and negative correlation at lower latitudes.[44] However, not all scientists accept this correlation as statistically significant, and some that do attribute it to other solar variability (e.g. UV or total irradiance variations) rather than directly to GCR changes.[46][47] Difficulties in interpreting such correlations include the fact that many aspects of solar variability change at similar times, and some climate systems have delayed responses.
Carbon-14 production
Sunspot record (blue) with 14C (inverted).The production of carbon-14 (radiocarbon: 14C) also is related to solar activity. Carbon-14 is produced in the upper atmosphere when cosmic ray bombardment of atmospheric nitrogen (14N) induces the Nitrogen to undergo β+ decay, thus transforming into an unusual isotope of Carbon with an atomic weight of 14 rather than the more common 12. Because cosmic rays are partially excluded from the Solar System by the outward sweep of magnetic fields in the solar wind, increased solar activity results in a reduction of cosmic rays reaching the Earth's atmosphere and thus reduces 14C production. Thus the cosmic ray intensity and carbon-14 production vary inversely to the general level of solar activity.[48]
Therefore, the atmospheric 14C concentration is lower during sunspot maxima and higher during sunspot minima. By measuring the captured 14C in wood and counting tree rings, production of radiocarbon relative to recent wood can be measured and dated. A reconstruction of the past 10,000 years shows that the 14C production was much higher during the mid-Holocene 7,000 years ago and decreased until 1,000 years ago. In addition to variations in solar activity, the long term trends in carbon-14 production are influenced by changes in the Earth's geomagnetic field and by changes in carbon cycling within the biosphere (particularly those associated with changes in the extent of vegetation since the last ice age).[49]
Global warming
See also: Global warmingSee also
References
Footnotes
- ^ Satellite observations of total solar irradiance
- ^ a b c Willson, Richard C.; H.S. Hudson (1991). "The Sun's luminosity over a complete solar cycle". Nature 351 (6321): 42–4. doi:10.1038/351042a0. http://www.nature.com/nature/journal/v351/n6321/abs/351042a0.html.
- ^ "Solar Forcing of Climate". Climate Change 2001: Working Group I: The Scientific Basis. http://www.grida.no/climate/ipcc_tar/wg1/244.htm. Retrieved 2005-03-10.
- ^ Weart, Spencer (2006). "The Discovery of Global Warming". In Weart, Spencer. American Institute of Physics. http://www.aip.org/history/climate/index.html. Retrieved 2007-04-14.
- ^ http://acrim.com/TSI%20Monitoring.htm
- ^ Willson, R. C.; Mordvinov, A. V. (2003). "Secular total solar irradiance trend during solar cycles 21–23". Geophys. Res. Lett. 30 (5): 1199. Bibcode 2003GeoRL..30e...3W. doi:10.1029/2002GL016038. http://www.agu.org/journals/gl/gl0905/2008GL036307.
- ^ "Construction of a Composite Total Solar Irradiance (TSI) Time Series from 1978 to present". Physikalisch-Meteorologisches Observatorium Davos (PMOD). http://www.pmodwrc.ch/pmod.php?topic=tsi/composite/SolarConstant. Retrieved 2005-10-05.
- ^ Committee on Surface Temperature Reconstructions for the Last 2,000 Years, Board on Atmospheric Sciences and Climate, Division on Earth and Life Studies, National Research Council of the National Academies. (2006). "Climate Forcings and Climate Models". In North, Gerald R.; Biondi, Franco; Bloomfield, Peter et al.. Surface Temperature Reconstructions for the Last 2,000 Years. National Academies Press. ISBN 0-309-10225-1. http://books.nap.edu/openbook.php?record_id=11676&page=102. Retrieved 19 April 2007.
- ^ Lean, J. (2000). "Evolution of the Sun's Spectral Irradiance Since the Maunder Minimum". Geophysical Research Letters 27 (16): 2425–8. Bibcode 2000GeoRL..27.2425L. doi:10.1029/2000GL000043. ftp://ftp.ncdc.noaa.gov/pub/data/paleo/climate_forcing/solar_variability/lean2000_irradiance.txt.
- ^ Scafetta, N.; West, B. J. (2006). "Phenomenological solar signature in 400 years of reconstructed Northern Hemisphere temperature record". Geophys. Res. Lett. 33 (17): L17718. Bibcode 2006GeoRL..3317718S. doi:10.1029/2006GL027142. http://www.agu.org/journals/gl/gl0617/2006GL027142/.
- ^ UCAR (September 13, 2006). "Changes In Solar Brightness Too Weak To Explain Global Warming". Press release. http://www.ucar.edu/news/releases/2006/brightness.shtml. Retrieved 18 April 2007.
- ^ "Great Moments in the History of Solar Physics 1". Great Moments in the History of Solar Physics. Archived from the original on March 1, 2006. http://web.archive.org/web/20060301083022/http://web.hao.ucar.edu/public/education/sp/great_moments.html. Retrieved 2006-03-19.
- ^ Arctowski, Henryk (1940). "On Solar Faculae and Solar Constant Variations" (PDF). Proc. Natl. Acad. Sci. U.S.A. 26 (6): 406–11. doi:10.1073/pnas.26.6.406. PMC 1078196. PMID 16588370. http://www.pnas.org/cgi/reprint/26/6/406.pdf.
- ^ Fritts, Harold C. (1976). Tree rings and climate. Boston: Academic Press. ISBN 0-12-268450-8.
- ^ "William Herschel (1738–1822)". High Altitude Observatory. Archived from the original on June 7, 2007. http://web.archive.org/web/20070607215435/http://www.hao.ucar.edu/Public/education/bios/herschel.html. Retrieved 2008-02-27.
- ^ Camp, Charles D.; Tung, Ka-Kit; Quinif, Yves; Kaufman, Olivier; Van Ruymbeke, Michel; Vandiepenbeeck, Marc; Camelbeeck, Thierry (2006). "The Influence of the Solar Cycle and QBO on the Late Winter Stratospheric Polar Vortex" (PDF). EOS Trans. AGU 87 (52): Fall Meet. Suppl., Abstract #A11B–0862. Bibcode 2006EOSTr..87..298V. doi:10.1029/2006EO300005. http://www.amath.washington.edu/research/articles/Tung/journals/camp-tung-0721-revised.pdf. Retrieved 28 April 2009.
- ^ TSI Composites
- ^ http://www.pmodwrc.ch/pmod.php?topic=tsi/composite/SolarConstant
- ^ Richard C. Willson, Alexander V. Mordvinov (2003). "Secular total solar irradiance trend during solar cycles 21–23". Geophysical Research Letters 30 (5): 1199. Bibcode 2003GeoRL..30e...3W. doi:10.1029/2002GL016038.
- ^ Steven DeWitte, Dominiqu Crommelynck, Sabri Mekaoui, and Alexandre Joukoff (2004). "MEASUREMENT AND UNCERTAINTY OF THE LONG-TERM TOTAL SOLAR IRRADIANCE TREND". Solar Physics 224 (1-2): 209–216. doi:10.1007/s11207-005-5698-7.
- ^ Fröhlich, C. and J. Lean (2004). "Solar Radiative Output and its Variability: Evidence and Mechanisms". Astronomy and Astrophysical Reviews 12 (4): 273–320. doi:10.1007/s00159-004-0024-1. 10.1007/s00159-004-0024-1.
- ^ Eddy, J.A. (1990). "Samuel P. Langley (1834–1906)". Journal for the History of Astronomy 21: 111–20. http://www.hao.ucar.edu/Public/education/bios/langley.html.
- ^ Foukal, P. V.; Mack, P. E.; Vernazza, J. E. (1977). "The effect of sunspots and faculae on the solar constant". The Astrophysical Journal 215: 952. Bibcode 1977ApJ...215..952F. doi:10.1086/155431. http://ucp.uchicago.edu/cgi-bin/resolve?id=doi:10.1086/155431.
- ^ a b c Willson RC, Gulkis S, Janssen M, Hudson HS, Chapman GA (February 1981). "Observations of Solar Irradiance Variability". Science 211 (4483): 700–2. doi:10.1126/science.211.4483.700. PMID 17776650. http://www.sciencemag.org/cgi/pmidlookup?view=long&pmid=17776650.
- ^ J. R. Hickey, B. M. Alton, H. L. Kyle and E. R. Major (1988). "Observation of total solar irradiance (TSI) variability from Nimbus satellites". Advances in Space Research 8 (7): 5–10. doi:10.1016/0273-1177(88)90164-0. http://www.sciencedirect.com/science?_ob=ArticleURL&_udi=B6V3S-472BJN2-8F&_user=10&_coverDate=12%2F31%2F1988&_rdoc=1&_fmt=high&_orig=search&_sort=d&_docanchor=&view=c&_searchStrId=1254179665&_rerunOrigin=google&_acct=C000050221&_version=1&_urlVersion=0&_userid=10&md5=affa6a3023aac8f07070df80fc72cce1.
- ^ Usoskin, Ilya G.; Solanki, Sami K.; Schüssler, Manfred; Mursula, Kalevi; Alanko, Katja (2003). "A Millennium Scale Sunspot Number Reconstruction: Evidence For an Unusually Active Sun Since the 1940’s". Physical Review Letters 91 (21): 211101. arXiv:astro-ph/0310823. Bibcode 2003PhRvL..91u1101U. doi:10.1103/PhysRevLett.91.211101.
- ^ Solanki, Sami K.; Usoskin, Ilya G.; Kromer, Bernd; Schüssler, Manfred; Beer, Jürg (2004). "Unusual activity of the Sun during recent decades compared to the previous 11,000 years" (PDF). Nature 431 (7012): 1084–7. doi:10.1038/nature02995. PMID 15510145. http://cc.oulu.fi/%7Eusoskin/personal/nature02995.pdf. Retrieved 17 April 2007. , "11,000 Year Sunspot Number Reconstruction". Global Change Master Directory. http://gcmd.nasa.gov/KeywordSearch/Metadata.do?Portal=GCMD&KeywordPath=%5BParameters%3ACategory%3D%27EARTH+SCIENCE%27%2CTopic%3D%27SUN-EARTH+INTERACTIONS%27%2CTerm%3D%27SOLAR+ACTIVITY%27%2CVariable%3D%27SUNSPOTS%27%5D&OrigMetadataNode=GCMD&EntryId=NOAA_NCDC_PALEO_2005-015&MetadataView=Brief&MetadataType=0&lbnode=gcmd3b. Retrieved 2005-03-11.
- ^ Usoskin, Ilya G.; Solanki, Sami K.; Kovaltsov, Gennady A. (2007). "Grand minima and maxima of solar activity: new observational constraints" (PDF). Astron. Astrophys. 471 (1): 301–9. Bibcode 2007A&A...471..301U. doi:10.1051/0004-6361:20077704. http://cc.oulu.fi/~usoskin/personal/aa7704-07.pdf.
- ^ Sonett, C. P.; Finney, S. A.; Berger, A. (April 24, 1990). "The Spectrum of Radiocarbon". Phil. Trans. R. Soc. Lon. A 330 (1615): 413–26.
- ^ a b Braun, H; Christl, M; Rahmstorf, S; Ganopolski, A; Mangini, A; Kubatzki, C; Roth, K; Kromer, B (10 November 2005). "Possible solar origin of the 1,470-year glacial climate cycle demonstrated in a coupled model". Nature 438 (7065): 208–11. doi:10.1038/nature04121. PMID 16281042. http://www.awi.de/fileadmin/user_upload/Research/Research_Divisions/Climate_Sciences/Paleoclimate_Dynamics/Modelling/Methods/PossibleSolar.pdf.
- ^ "The Sun and Climate" (PDF). U.S. Geological Survey. Fact Sheet 0095-00. http://pubs.usgs.gov/fs/fs-0095-00/fs-0095-00.pdf.
- ^ Vasiliev, S. S.; Dergachev, V. A. (2002). "The ~ 2400-year cycle in atmospheric radiocarbon concentration: bispectrum of 14C data over the last 8000 years". ANGEO 20 (1): 115–20. http://www.ann-geophys.net/20/115/2002/angeo-20-115-2002.pdf.
- ^ Xapsos, M. A.; Burke, E. A. (July 2009). "Evidence of 6 000-Year Periodicity in Reconstructed Sunspot Numbers". Solar Physics 257 (2): 363–9. doi:10.1007/s11207-009-9380-3.
- ^ Scafetta, Nicola; West, Bruce J. (2005). "Estimated solar contribution to the global surface warming using the ACRIM TSI satellite composite" (PDF). Geophysical Research Letters 32 (18): L18713. Bibcode 2005GeoRL..3218713S. doi:10.1029/2005GL023849. http://www.fel.duke.edu/~scafetta/pdf/2005GL023849.pdf.
- ^ Perry, Charles A.; Hsu, Kenneth J. (2000). "Geophysical, archaeological, and historical evidence support a solar-output model for climate change" (PDF). Proc. Natl. Acad. Sci. U.S.A. 97 (23): 12433–8. doi:10.1073/pnas.230423297. PMC 18780. PMID 11050181. http://www.pnas.org/cgi/reprint/97/23/12433.pdf.
- ^ Hathaway, David H.; Wilson, Robert M. (2004). "What the Sunspot Record Tells Us About Space Climate" (PDF). Solar physics 224 (1–2): 5–19. doi:10.1007/s11207-005-3996-8. Archived from the original on January 4, 2006. http://web.archive.org/web/20060104223339/http://science.msfc.nasa.gov/ssl/pad/solar/papers/hathadh/HathawayWilson2004.pdf. Retrieved 19 April 2007.
- ^ "Solar Variability: climatic change resulting from changes in the amount of solar energy reaching the upper atmosphere.". Introduction to Quaternary Ecology. http://www.geo.arizona.edu/palynology/geos462/20climsolar.html. Retrieved 2005-03-11.
- ^ Board on Global Change, Commission on Geosciences, Environment, and Resources, National Research Council. (1994). Solar Influences on Global Change. Washington, D.C: National Academy Press. p. 36. ISBN 0-309-05148-7. http://books.nap.edu/openbook.php?record_id=4778&page=R1.
- ^ Wang, Y.-M.; Lean, J. L.; Sheeley, N. R. (2005). "Modeling the Sun's magnetic field and irradiance since 1713". The Astrophysical journal 625 (1): 522–38. Bibcode 2005ApJ...625..522W. doi:10.1086/429689. http://www.climatesci.org/publications/pdf/Wang_2005.pdf.
- ^ Krivova, N. A.; Balmaceda, L.; Solanki, S. K. (2007). "Reconstruction of solar total irradiance since 1700 from the surface magnetic flux". A&A 467 (1): 335–46. Bibcode 2007A&A...467..335K. doi:10.1051/0004-6361:20066725. http://www.aanda.org/articles/aa/abs/2007/19/aa6725-06/aa6725-06.html.
- ^ Steinhilber, F.; Beer, J.; Fröhlich, C. (2009). "Total solar irradiance during the Holocene". Geophys. Res. Lett. 36 (19): L19704. Bibcode 2009GeoRL..3619704S. doi:10.1029/2009GL040142.
- ^ Lean, J. (14 April 1989). "Contribution of Ultraviolet Irradiance Variations to Changes in the Sun's Total Irradiance Science"]. Science 244 (4901): 197–200. doi:10.1126/science.244.4901.197. PMID 17835351. http://www.sciencemag.org/cgi/content/abstract/244/4901/197. "1 percent of the sun's energy is emitted at ultraviolet wavelengths between 200 and 300 nanometers, the decrease in this radiation from 1 July 1981 to 30 June 1985 accounted for 19 percent of the decrease in the total irradiance". (19% of the 1/1366 total decrease is 1.4% decrease in UV)
- ^ Damon, Paul E.; Paul Laut (28 2004). "Pattern of Strange Errors Plagues Solar Activity and Terrestrial Climate Data" (PDF). Eos 85 (39September): 370–4. Bibcode 2004EOSTr..85..370D. doi:10.1029/2004EO390005. http://stephenschneider.stanford.edu/Publications/PDF_Papers/DamonLaut2004.pdf. Retrieved October 5, 2005.
- ^ a b Tinsley, Brian A.; Yu, Fangqun (2004). "Atmospheric Ionization and Clouds as Links Between Solar Activity and Climate". In Pap, Judit M.; Fox, Peter. Solar Variability and its Effects on Climate. 141. American Geophysical Union. pp. 321–339. ISBN 0-87590-406-8. http://www.utdallas.edu/physics/pdf/Atmos_060302.pdf. Retrieved 19 April 2007.
- ^ Svensmark, Henrik (1998). "Influence of Cosmic Rays on Earth's Climate" (PDF). Physical Review Letters 81 (22): 5027–5030. Bibcode 1998PhRvL..81.5027S. doi:10.1103/PhysRevLett.81.5027. http://www.cosis.net/abstracts/COSPAR02/00975/COSPAR02-A-00975.pdf. Retrieved 19 April 2007.
- ^ E. Pallé, C.J. Butler, K. O'Brien (2004). "The possible connection between ionization in the atmosphere by cosmic rays and low level clouds" (PDF). Journal of Atmospheric and Solar-Terrestrial Physics 66 (18): 1779. doi:10.1016/j.jastp.2004.07.041. http://www.arm.ac.uk/preprints/433.pdf.
- ^ Pallé, E. (2005). "Possible satellite perspective effects on the reported correlations between solar activity and clouds" (PDF). Geophysical Research Letters 32 (3): L03802.1–4. Bibcode 2005GeoRL..3203802P. doi:10.1029/2004GL021167. http://bbso.njit.edu/Research/EarthShine/literature/Palle_2005_GRL.pdf.
- ^ "Astronomy: On the Sunspot Cycle". http://users.zoominternet.net/~matto/M.C.A.S/sunspot_cycle.htm. Retrieved 2008-02-27.
- ^ Landscheidt, Theodor (21 September 2003). "Variations in CO2 Growth Rate Associated with Solar Activity". John-daly.com — website of John Lawrence Daly. http://www.john-daly.com/theodor/co2new.htm. Retrieved 2007-04-19.
- ^ "Climate Change 2001: The Scientific Basis". http://www.grida.no/climate/ipcc_tar/wg1/122.htm. Retrieved 2005-10-05.
- ^ Shaviv, Nir J.; Veizer, Ján (2003). "Celestial driver of Phanerozoic climate?" (PDF). GSA Today 13 (7): 4–10. doi:10.1130/1052-5173(2003)013<0004:CDOPC>2.0.CO;2. http://www.gsajournals.org/archive/1052-5173/13/7/pdf/i1052-5173-13-7-4.pdf. Retrieved 19 April 2007.
- ^ "http://www.soest.hawaii.edu/GG/FACULTY/POPP/Rahmstorf%20et%20al.%202004%20EOS.pdf" (PDF). http://www.soest.hawaii.edu/GG/FACULTY/POPP/Rahmstorf%20et%20al.%202004%20EOS.pdf. Retrieved 2005-10-05.
General references
- Abbot, C. G. (1966). "Solar Variation, A Weather Element" (PDF). Proc. Natl. Acad. Sci. U.S.A. 56 (6): 1627–34. doi:10.1073/pnas.56.6.1627. PMC 220145. PMID 16591394. http://www.pnas.org/cgi/reprint/56/6/1627.pdf.
- Willson, Richard C.; H.S. Hudson (1991). "The Sun's luminosity over a complete solar cycle". Nature 351 (6321): 42–4. doi:10.1038/351042a0. http://www.nature.com/nature/journal/v351/n6321/abs/351042a0.html.
- "The Sun and Climate". U.S. Geological Survey Fact Sheet 0095-00. http://pubs.usgs.gov/fs/fs-0095-00/. Retrieved 2005-02-21.
- "The Sun's role in Climate Changes" (PDF). Proc. of The International Conference on Global Warming and The Next Ice Age, 19–24 August 2001, Halifax, Nova Scotia.. Archived from the original on October 22, 2004. http://web.archive.org/web/20041022012450/http://zeus.nascom.nasa.gov/~pbrekke/articles/halifax_brekke.pdf. Retrieved 2005-02-21.
- White, Warren B.; Lean, Judith; Cayan, Daniel R.; Dettinger, Michael D. (1997). "Response of global upper ocean temperature to changing solar irradiance". Journal of Geophysical Research 102 (C2): 3255–66. Bibcode 1997JGR...102.3255W. doi:10.1029/96JC03549. http://www.agu.org/pubs/crossref/1997/96JC03549.shtml.
- Foukal, Peter; et al. (1977). "The effects of sunspots and faculae on the solar constant". Astrophysical Journal 215: 952. Bibcode 1977ApJ...215..952F. doi:10.1086/155431.
- Dziembowski, W.A.; P.R. Goode, and J. Schou (2001). "Does the sun shrink with increasing magnetic activity?". Astrophysical Journal 553 (2): 897–904. Bibcode 2001ApJ...553..897D. doi:10.1086/320976.
- Stetson, H.T. (1937). Sunspots and Their Effects. New York: McGraw Hill.
External links
- Gerrit Lohmann, Norel Rimbu, Mihai Dima (2004). "Climate signature of solar irradiance variations: analysis of long-term instrumental, historical, and proxy data". International Journal of Climatology 24 (8): 1045–56. doi:10.1002/joc.1054. http://www3.interscience.wiley.com/cgi-bin/abstract/109062443/ABSTRACT.
- Solar Climatic Effects (Recent Influence) — Summary. Center for the Study of Carbon Dioxide and Global Change. 19 March 2003. http://www.co2science.org/subject/s/summaries/solarrecin.htm
- NOAA / NESDIS / NGDC (2002) Solar Variability Affecting Earth NOAA CD-ROM NGDC-05/01. This CD-ROM contains over 100 solar-terrestrial and related global data bases covering the period through April 1990. http://www.ngdc.noaa.gov/stp/CDROM/solar_variability.html
- Solanki, S.K.; Fligge, M. (2001). Long-term changes in solar irradiance. ESA Publications Division. ESA SP-463. http://www.astro.phys.ethz.ch/papers/fligge/solspa_2.pdf.
- Solanki, S.K.; Fligge, M. (2000). "Reconstruction of past solar irradiance". Space Science Review 94 (1/2): 127–38. doi:10.1023/A:1026754803423. http://www.astro.phys.ethz.ch/papers/fligge/solfli_rev.pdf.
- Reid, George C. (1995). "The sun-climate question: Is there a real connection?". Rev. Geophys. 33 (Suppl). http://www.agu.org/revgeophys/reid00/reid00.html. Aeronomy Laboratory, NOAA/ERL, Boulder, Colorado. U.S. National Report to IUGG, 1991–1994
- Recent Total Solar Irradiance data updated every Monday
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Categories: Periodic phenomena | Climate change | Solar phenomena | Climate forcing agents
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