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PhysicsThe Sun and space weatherInteractive 3D 12 min

From the Sun’s core to the auroras

Open up the Sun, follow energy transfers to Earth and explore what makes auroras glow.

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What you can change

Variables

  • Depth probe: move from the centre to 2 R☉, or two solar radii, and read temperature in kelvin and mass density in g/cm³.
  • Photon mean free path: from 0.005 to 1 cm between interactions, to explore the estimated diffusion time.
  • Solar cycle phase: from minimum to maximum activity, changing the active regions.
  • CME speed: set a coronal mass ejection to 400–3,200 km/s and compare its estimated arrival time.
  • Bz field: its north–south component ranges from −40 to +15 nT. A southward field favours energy transfer into the magnetosphere.
  • Wind density: vary the number of protons per cm³ and observe the magnetopause position. Also compare the illustrative auroral latitude and storm G scale as wind and field settings change.
  • Display: show or hide layers, open the cutaway, enable field lines and compare visible, UV, magnetic-field and thermal views.
Orders of magnitude

Key figures

≈ 15 million K
temperature at the Sun’s centre
≈ 170,000 years
model-dependent estimate of energy diffusion time
≈ 8 min 20 s
light travel time to Earth
≈ 1–2 million K
ordinary coronal temperature
≈ 100–300 km
indicative auroral altitude, with red possible higher up
Understand

What happens, step by step.

  1. 01

    Fusion, then a long journey

    At the Sun’s centre, at about 15 million kelvin, successive reactions turn hydrogen nuclei into helium. A small part of their mass becomes energy. Neutrinos escape almost freely, while photons are absorbed, re-emitted and scattered. The roughly 170,000-year diffusion time is a model-dependent estimate: we are not following one intact photon. Once light escapes, it reaches Earth in about 8 min 20 s.

  2. 02

    Layers and a dynamo

    In the radiative zone, photon interactions carry energy. Farther out, plasma rises, cools and sinks: this is convection. Near their junction, the tachocline links regions rotating at different rates. Plasma motions sustain the magnetic field through a mechanism called a dynamo. The tachocline’s precise role remains debated. Sunspots mark cooler regions where the field reduces convection. The activity cycle lasts about 11 years, with a variable duration.

  3. 03

    A hotter atmosphere

    The photosphere releases the Sun’s white visible light. Above it, the chromosphere hosts jets and the transition region marks a sharp temperature rise. The corona commonly reaches about 1–2 million kelvin but remains very thin. Waves, turbulence and field rearrangements contribute to heating; their relative roles remain under study. The corona extends into the solar wind. Fast wind comes mainly from coronal holes; slow wind has several origins.

  4. 04

    Several clocks to Earth

    A flash of light, solar energetic particles and a CME are distinct phenomena that sometimes occur together. Light takes about 8 min 20 s; fast particles often arrive in 20 min to a few hours. A CME commonly takes 1–3 days, sometimes 15–18 h, and can miss Earth. Ordinary wind is continuous: about 4.3 days at 400 km/s. Near L1, between Sun and Earth, satellites measure the wind and its field, often giving a further 15–60 min of warning.

  5. 05

    From Earth’s field to the auroras

    The wind meets a bow shock, then the magnetopause bounding the region dominated by Earth’s field. Higher pressure compresses this boundary. A southward interplanetary field favours reconnection: fields rearrange and energy enters the magnetosphere. The nightside tail can store and release it. Electrons excite atmospheric oxygen and nitrogen, which emit auroral light. Storms can also disrupt satellites and power grids.

  6. 06

    How do we know the Sun?

    The interior has never been photographed. Helioseismology uses vibrations measured at the surface to constrain interior models. Neutrinos reveal fusion directly: Borexino detected those from the CNO cycle in 2020, with final results in 2023. Telescopes distinguish structures through different kinds of light. Parker measures plasma close to the Sun; Solar Orbiter viewed its poles from outside the orbital plane in 2025. Satellites near L1 link these observations to conditions heading towards Earth.

Check

What the scene simplifies

  • Atmospheric layers are enlarged and distances change scale. Boundaries are guides: a conventional core, a tachocline overlapping the radiative zone and a dynamic atmosphere.
  • Playback durations are not physical times. Energy transfers do not follow one particle from core to aurora. The diffusion model assumes a constant mean free path.
  • The radial probe gives orders of magnitude: a resampled solar Model S, a VAL-C atmosphere and a quiet corona joined for teaching. The corona uses a constant reference temperature and a density conversion assuming fully ionised hydrogen only.
  • The Sun is white in visible light. UV and thermal palettes are display conventions. Field lines are not luminous wires.
  • The CME calculation assumes uniform wind and fixed drag beyond 20 R☉. The initial journey is added at constant speed. Initial acceleration, direction, width and interactions between ejections are not modelled; the arrival time is not a forecast.
  • The magnetopause follows an average empirical model. Kp and auroral latitude are rough illustrations, without wind history or magnetic local time. The derived G scale does not predict an event’s precise effects; Kp, G and Dst are not interchangeable.
Sources

Further reading

  1. NASA Marshall — The Solar Interior
  2. IAU 2015 — Nominal conversion constants
  3. NASA — Ancient Sunlight
  4. Stix (2003) — On the time scale of energy transport in the Sun
  5. Christensen-Dalsgaard (2021) — Solar structure and evolution
  6. Borexino (2020) — CNO solar neutrinos
  7. Borexino (2023) — Final results on CNO solar neutrinos
  8. NASA — Sun: Facts
  9. NASA SVS — Fast and Slow Solar Wind
  10. ESA — Solar Orbiter, first views of the poles (2025)
  11. NASA — STEREO Science Guide
  12. NOAA — Coronal Mass Ejections
  13. NOAA — NOAA Goes to L1 with DSCOVR
  14. NOAA — Earth’s magnetosphere
  15. NASA — Auroras
  16. NOAA — Space Weather Scales
  17. Model S — Christensen-Dalsgaard et al. (1996)
  18. VAL-C — Czech Academy of Sciences
  19. Wexler et al. (2019) — Coronal electron density
  20. Dumbović et al. (2021) — Drag-Based Model Tools
  21. Shue et al. (1998) — Magnetopause location