Mindmap
Lecture 20: Solar Variability
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Lecture 20: Solar Variability
Sunspots and solar radiation
- High sunspot abundance = strong solar emissions.
- From the Sun's polar regions and bright margins of sunspots.
- Sunspots
- Temporary features visible on the Sun's surface.
- Caused by slightly lower temperatures that reflect concentrations of magnetic flux inhibiting convection.
- The brighter area around sunspots represent solar flares that are responsible for altering the total radiation emitted by the sun.
- Occur over an 11-year cycle (known as the solar cycle).
- Defined by astronomer Rudolf Wolf.
- Cycle 1 is between 1755-1766.
- We are currently reaching the end of cycle 24.
- Defined by astronomer Rudolf Wolf.
- High sunspot abundance = strong solar emissions.
Sunspot cycles
- Cause 0.1% variability in total irradiance output.
- Vary over time.
- First observed by Spörer and Maunder during the Maunder Minimum (1645-1715).
- The Maunder Minimum was a period of low sunspot activity.
The radiation spectrum
- There are changes in the spectrum of radiation emitted during these cycles.
- Extreme Ultra Violet radiation (EUV) peaks at the solar maxima, increasing by 10%.
- There are changes in the spectrum of radiation emitted during these cycles.
Long-term sunspot cycles
- The solar index has been constructed to cover the last 12,000 years.
- Data used in climate models.
- The solar index has been constructed to cover the last 12,000 years.
Cosmogenic isotopes
- Cosmic rays were first visualised using cloud chambers, which display ionising particles.
- The radiocarbon timescale is calibrated using dendrochronology (by lining up tree rings).
- Ice core records also contain evidence supporting solar variability in the form of cosmogenic isotopes beryllium-10 and carbon-14.
- Carbon-14 production varied with the solar index throughout history.
- Given that cosmic particles are required to form carbon-14, having a weaker magnetic field leads to faster carbon-14 production.
- Weaker magnetic field = weaker solar shielding = more bombardment by cosmic particles = faster carbon-14 production.
- This is largely controlled by a 420-year cycle.
- Carbon-14 cycle
- 1. Carbon-14 forms in the upper atmosphere when free neutrons collide with nitrogen-14 (a cosmic particle).
- 2. Because it is an unstable isotope, nitrogen-14 undergoes radioactive decay and forms carbon-14.
- This occurs over ~15,000 years.
- Beta particles are emitted during decay.
- 3. Carbon-14 is oxidised into carbon(-14) dioxide which mixes with carbon(-12) dioxide through the atmosphere and hydrosphere.
- It is then incorporated into the biosphere (e.g. via photosynthesis).
- Organisms cannot ingest neat carbon-14.
- 4. Carbon-14 is incorporated into plants. When they die, carbon-14 begins to decay back into nitrogen.
- So scientists measure how much C-14 remains in an object to estimate its age.
Climate
- The 'hockey stick curve' shows temperatures over the last millennium (1000 years).
- Temperature records are reflected in shell increments and tree rings.
- Temperature records also partly line up with solar variability records (as temperature is also affected by other factors).
- The 'hockey stick curve' shows temperatures over the last millennium (1000 years).
The Little Ice Age
- Took place approximately between 1500 and 1900.
- A period of high Icelandic sea ice coverage.
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- Year 1 Earth Systems Science Mindmap am Lecture 20: Solar Variability, erstellt von Amber Hawkins am 19/11/2024.
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- Amber Hawkins
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