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How the Sun’s “seasons” affect our planet’s atmosphere

Pierre Henriquet
Pierre Henriquet
Doctor in Nuclear Physics and Columnist at Polytechnique Insights
Key takeaways
  • The Sun has an impact on its immediate environment and on more distant planets, but also on the entire region of space surrounding our Solar System, which is called the heliosphere.
  • There are various consequences of the interaction of this flow of solar particles with the Earth's magnetosphere; one of the most beautiful being the Northern Lights.
  • A negative consequence of this permanent bombardment is it that it can prematurely age satellites and even lead to them failing because they are highly exposed to solar wind particles in orbit.
  • The Sun's extremely high temperature allows for the formation of bubbles that 'burst' its atoms into a soup of nuclei and free electrons. This 'plasma' is very sensitive to electric and magnetic fields.
  • Solar activity evolves periodically in a long cycle of about 11.5 years, passing through a maximum of activity and a minimum. These can be referred to as the Sun's 'seasons'.

Eve­ry 11.5 years, the Sun goes through a per­iod of par­ti­cu­lar­ly intense acti­vi­ty. It is cha­rac­te­ri­sed by strong solar wind, lea­ding to more frequent satel­lite fai­lures due to a bom­bard­ment of par­ticles from the Sun. But whe­ther solar acti­vi­ty is high or low, life is tough for tech­no­lo­gies in orbit. The Sun has an impact on its imme­diate envi­ron­ment, on the more dis­tant pla­nets, but also on the whole region of space sur­roun­ding our Solar Sys­tem, which is cal­led the heliosphere.

What are the consequences for space activities ?

The conse­quences of the inter­ac­tion of this flow of solar par­ticles with the Ear­th’s magne­tos­phere – our pla­net’s magne­tic field – are nume­rous and varied. One of the most beau­ti­ful is, of course, the auro­ras in the nor­thern and sou­thern hemis­pheres (auro­ra borea­lis and aus­tra­lis res­pec­ti­ve­ly). At the poles, a small frac­tion of the solar wind can cross the magne­tos­phere (see image of the Ear­th’s magne­tic field below) and vio­lent­ly inter­act with the Ear­th’s atmos­phere. This trans­fer of ener­gy excites the rare­fied atoms and mole­cules at the top of the atmos­phere, which re-emits it in the form of magni­ficent drapes of light.

Magne­tic field lines sur­roun­ding the Earth. In colour : solar wind den­si­ty. (The Sun is on the left of the image) © NASA

Other conse­quences are more pro­ble­ma­tic. Satel­lites in orbit around our pla­net are high­ly expo­sed to solar wind par­ticles. This per­ma­nent bom­bard­ment is one of the main rea­sons for the ageing or pos­sible fai­lure of these satel­lites. Like the irra­dia­tion pro­cesses used in indus­try on Earth, the mecha­ni­cal, elec­tri­cal and/or opti­cal pro­per­ties of satel­lite com­po­nents is gra­dual­ly alte­red. Tran­sient or per­ma­nent fai­lures of the on-board elec­tro­nics may also occur (more fre­quent­ly, of course, during solar maxi­mum per­iods). The­re­fore, they must often be shiel­ded, and their elec­tro­nics rein­for­ced to bet­ter withs­tand solar radiation.

Ground tech­no­lo­gies can also be affec­ted by the solar cycle. While the Sun’s tem­pe­ra­ture and light inten­si­ty do not change during the solar cycle (it does not get hot­ter eve­ry 11.5 years), the geo­ma­gne­tic storms cau­sed by a coro­nal mass ejec­tion ente­ring the Ear­th’s envi­ron­ment can be so intense that huge indu­ced elec­tri­cal cur­rents appear in the Ear­th’s power grid. In 1989, for example, a wides­pread power fai­lure brought Cana­da to a stand­still for nine hours. The entire net­work col­lap­sed in just 25 seconds. This is pro­ble­ma­tic as our civi­li­sa­tion is beco­ming ever more dependent on electricity…

The Sun makes bubbles

Astro­no­mers have long sought to cha­rac­te­rise the so-cal­led helios­phere, which limits two zones of space : the inter­ior, domi­na­ted by the solar wind, and the exte­rior, made up of par­ticles in the inter­stel­lar medium. Since the Sun emits solar wind par­ticles in a glo­bal­ly iso­tro­pic man­ner, its shape was ini­tial­ly ima­gi­ned as an elon­ga­ted « bubble » sur­roun­ding the solar sys­tem. Howe­ver, a recent paper1 sug­gests, based on exten­sive nume­ri­cal simu­la­tions and sky obser­va­tions, that the helios­phere of our Solar Sys­tem is sha­ped like… a crois­sant ! This is due to the com­plex inter­ac­tions bet­ween the hydro­gen atoms in the inter­stel­lar medium and the char­ged par­ticles emit­ted by the Sun.

The ‘crois­sant’ pro­du­ced by the latest nume­ri­cal simu­la­tions of the helios­phere. © NASA

The shape of this helios­phere will obvious­ly depend on the com­po­si­tion, den­si­ty, and speed of the flow of par­ticles coming from the Sun. Eve­ry second, the Sun loses about 1 mil­lion tonnes of elec­trons, hydro­gen nuclei and helium in a ‘wind’ that spreads around it, bathing the pla­nets and other bodies as far as the edges of the Solar Sys­tem. It is, for example, this solar wind that shapes one of the two types of tails of comets by car­rying the dust and gas par­ticles ejec­ted from the comets’ nuclei away from the Sun.

Comet C/2021 A1 (Leo­nard) ima­ged by Dan Bart­lett at the begin­ning of Decem­ber 2021

This solar wind also inter­acts with the pla­nets of the Solar Sys­tem, more or less direct­ly, depen­ding on the pre­sence or absence of a magne­tic field around them. The very high tem­pe­ra­ture of the Sun ‘explodes’ its atoms into a soup of nuclei and free elec­trons, cal­led a ‘plas­ma’, which is very sen­si­tive to elec­tric and magne­tic fields. So, when these par­ticles arrive near Earth, its magne­tic field will divert a signi­fi­cant por­tion of them and deflect the par­ticle sho­wer before it can irra­diate and ste­ri­lise the Ear­th’s surface.

Solar cycles and space weather

What are the pro­per­ties of the Sun’s ‘wind’ of par­ticles ? Is the wind constant ? Regu­lar ? Or do ‘solar wind storms’ exist ? Also, are there, as on Earth, ‘sea­sons’ when the solar wind is more intense ? The ans­wer to both of these ques­tions is yes.

Just as the sea­sons on Earth reap­pear regu­lar­ly each year, solar acti­vi­ty (which includes all the phe­no­me­na that occur on the sur­face of the Sun and around it) also evolves per­io­di­cal­ly in a long cycle of about 11.5 years.

Evo­lu­tion (obser­ved et simu­la­ted) of the solar cycle bet­ween 1995 et 2035. © NASA

During this cycle, the Sun goes through a maxi­mum of acti­vi­ty (the solar wind will be on ave­rage den­ser and fas­ter) and a mini­mum. This varia­tion in acti­vi­ty is not limi­ted to the amount of solar wind par­ticles, howe­ver. The Sun also regu­lar­ly pro­duces erup­tive phe­no­me­na cal­led coro­nal mass ejec­tions. These very intense bursts of solar par­ticles are pro­du­ced in very local regions on the sur­face of our star and are also ejec­ted radial­ly, at great dis­tances from the Sun.

When the Earth finds itself in this direc­tion, a par­ti­cu­lar­ly dense ‘wave’ of par­ticles arrives two to three days after the start of the ejec­tion. This wave of par­ticles joins the clas­sic solar wind for seve­ral hours. It is obvious­ly during the years of maxi­mum solar acti­vi­ty that the pro­ba­bi­li­ty of these power­ful erup­tive phe­no­me­na pro­du­cing ‘geo­ma­gne­tic storms’ in the Ear­th’s envi­ron­ment is greatest.

It would be wrong, howe­ver, to think that space acti­vi­ties are quie­ter during solar mini­mum per­iods. The solar wind is less dense and there are fewer solar flares, but other phe­no­me­na take centre stage. For example, the Ear­th’s atmos­phere also varies accor­ding to the ‘pres­sure’ of the solar wind. At solar mini­mum, the pres­sure is lower and the atmos­phere extends fur­ther into space. This puts aero­dy­na­mic stresses on low-orbi­ting satel­lites and signi­fi­cant­ly reduces their life span.

To conclude, our star signi­fi­cant­ly influences the Ear­th’s envi­ron­ment. Its plas­ma fin­gers caress us night and day, and it is through unders­tan­ding the com­plex inter­ac­tions bet­ween the Sun and the Earth that huma­ni­ty will be able to conti­nue to unders­tand space.

For more information, you can watch this ARTE video with Tahar Amari from the Center for Theoretical Physics at Ecole Polytechnique :

1« A Tur­bu­lent Helio­sheath Dri­ven by the Rayleigh–Taylor Insta­bi­li­ty » —The Astro­phy­si­cal Jour­nal, Volume 922, Num­ber 2 – https://doi.org/10.3847/1538–4357/ac2d2e

Contributors

Pierre Henriquet

Pierre Henriquet

Doctor in Nuclear Physics and Columnist at Polytechnique Insights

After a doctorate in Nuclear Physics applied to Medicine and a university degree in Astronomy/Astrophysics, Pierre Henriquet worked for 10 years at the Planetarium of the city of Vaulx-en-Velin where he perfected his talents as a science communicator with multiple audiences, both novices and specialists. Today, he is a freelance writer and mediator of science.

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