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Source-Region Properties and Sun–Earth Transit Kinematics of Geoeffective Coronal Mass Ejections Across Solar Cycles 23–25

This study statistically analyzes 177 geoeffective coronal mass ejections across solar cycles 23–25 to characterize their source-region properties and Sun–Earth transit kinematics, revealing that storm intensity is primarily driven by interplanetary magnetic field strength and duration rather than flare magnitude, while also identifying a westward source bias and a hyperbolic relationship between CME speed and transit time.

Original authors: Saurabh Tripathi, Tanmoy Samanta, Jayant Joshi, Vaibhav Pant

Published 2026-09-15
📖 6 min read🧠 Deep dive

Original authors: Saurabh Tripathi, Tanmoy Samanta, Jayant Joshi, Vaibhav Pant

Original paper licensed under CC BY 4.0 (https://creativecommons.org/licenses/by/4.0/). ✨ This is an AI-generated explanation of the paper below. It is not written or endorsed by the authors. For technical accuracy, refer to the original paper. Read full disclaimer

The Sun is a restless star, constantly shedding a stream of charged particles known as the solar wind. Occasionally, the Sun unleashes something far more violent: a coronal mass ejection. Imagine a billion tons of superheated gas, trapped in a magnetic bubble, suddenly ripped from the solar surface and hurled into space at millions of miles per hour. When these massive clouds are aimed directly at Earth, they can trigger geomagnetic storms. These storms are not merely auroral displays; they are powerful disturbances that can disrupt satellites, scramble radio communications, and even damage power grids on the ground. For decades, scientists have tried to predict exactly which eruptions will cause trouble and how severe the impact will be, but the journey from the Sun to Earth is complex. The magnetic fields inside these clouds can change, the clouds can slow down or speed up, and the path they take is influenced by the invisible magnetic highways of the solar system.

A new study by researchers at the Indian Institute of Astrophysics and the Indian Institute of Technology Delhi has taken a fresh look at this journey. By analyzing nearly 180 specific events where solar eruptions hit Earth over the last three solar cycles, the team mapped out the entire trip, from the moment the explosion began on the Sun to the moment it slammed into our planet's magnetic shield. They wanted to solve a few persistent puzzles: How fast do these clouds really travel? Does the size of the explosion on the Sun tell us how bad the storm will be on Earth? And where on the Sun do the most dangerous eruptions tend to come from?

The researchers built their picture using a vast collection of data from multiple spacecraft. They tracked the eruptions as they left the Sun using telescopes that watch the solar atmosphere, and then followed them all the way to Earth using sensors floating in space between our planet and the Sun. By matching the specific clouds that arrived at Earth with the eruptions that started them, they created a detailed timeline for each event. They found that the journey is not a simple, straight shot at a constant speed. On average, it takes about 62 hours for a coronal mass ejection to travel from the Sun to Earth, followed by another 15 hours before the full force of the magnetic storm hits our planet. This means that from the first sign of an eruption, there is roughly a three-day window before the peak of the geomagnetic disturbance.

One of the most significant findings concerns how we measure speed. Scientists have long debated which speed measurement best represents the true motion of these clouds. The study compared three different ways of measuring the speed of the cloud as it arrived at Earth: the speed of the shock wave at the front, the average speed of the magnetic core, and the maximum speed recorded anywhere within the cloud. The results showed that the maximum speed recorded during the entire passage of the cloud was the best indicator of how fast the cloud was moving when it left the Sun. This specific measurement allowed the researchers to reconstruct the timeline of the journey with the greatest accuracy, suggesting that looking for the peak speed within the arriving cloud gives the clearest picture of its original launch.

The study also challenged a common assumption about the relationship between the size of a solar flare and the severity of the resulting storm. A solar flare is a burst of radiation that often accompanies these eruptions, and it is easy to assume that a bigger flare means a bigger storm. However, the data showed only a weak connection between the brightness of the flare and the intensity of the magnetic storm on Earth. A massive flare does not guarantee a devastating storm, and a modest flare can sometimes trigger a severe one. Instead, the true driver of the storm's intensity was found to be the magnetic field inside the cloud. Specifically, the strength and duration of the southward-pointing magnetic field were the critical factors. If the magnetic field inside the cloud points in the opposite direction to Earth's magnetic field and stays that way for a long time, it allows energy to pour into our planet's magnetic shield, creating a powerful storm. This means that even a cloud traveling at a moderate speed can cause a major disaster if it carries a strong, sustained southward magnetic field.

The location of the eruption on the Sun also matters significantly. The researchers discovered a clear pattern in where these dangerous clouds come from. About 62 percent of the geoeffective eruptions originated in the western half of the Sun's visible disk, while only 38 percent came from the eastern half. This westward preference was even stronger for the fastest clouds. This asymmetry is likely due to the way the Sun's magnetic field is shaped, creating a natural path that connects the western side of the Sun more easily to Earth. Furthermore, the study noted that some of the most intense storms in recent history occurred not during the peak of solar activity, but during the declining phase of the solar cycle. This suggests that as the Sun's global magnetic field rearranges itself after a peak, the conditions for creating powerful, Earth-directed storms may actually improve, even as the total number of eruptions decreases.

Ultimately, this research provides a clearer map of how solar eruptions evolve into terrestrial storms. It confirms that predicting the impact of a solar eruption requires looking beyond the initial explosion on the Sun. The true danger lies in the magnetic structure of the cloud as it travels through space and the specific direction of its magnetic field when it arrives. By understanding that the maximum speed within the cloud is the best guide for its journey, and that the duration of the southward magnetic field is the key to storm intensity, scientists can refine their models for space weather. This work does not solve the problem of prediction entirely, but it offers a more reliable set of tools to understand the complex physics that governs the space between the Sun and Earth.

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