Showing posts with label Kelvin–Helmholtz instability. Show all posts
Showing posts with label Kelvin–Helmholtz instability. Show all posts

Thursday, October 22, 2026

A Magnetar Can Be Born When Two Neutron Stars Touch

>Illustration of a binary neutron star merger just as the two stars make contact. Credit: NASA/Goddard Space Flight Center



All neutron stars have intense magnetic fields. The typical magnetic field of a neutron star is about 100,000 times stronger than the strongest magnetic fields we can create on Earth. But about 1% of neutron stars have even stronger magnetic fields. Known as magnetars, their magnetic fields can be 1,000 times stronger than a regular magnetic field. They are a likely cause for powerful transient events such as soft gamma-ray repeaters and fast radio bursts. A new study looks at how magnetars might form.

The work focuses on the mergers of binary neutron stars. Often when two neutron stars collide they form a black hole. This is because the combined mass of the two neutron stars is greater than the Tolman-Oppenheimer-Volkoff (TOV) limit, which is around 2.6 solar masses. Most neutron stars are more massive than white dwarfs, which have a Chandrasekhar limit of about 1.4 solar masses. But some neutron stars have smaller masses. If they happen to have a total mass less than the TOV limit, then they can merge and become a single neutron star.

Using high-resolution simulations run on the Japanese supercomputer FUGAKU, the team looked at the merger of low-mass neutron star binaries. To simplify things a bit, they assumed stars with identical masses, but otherwise just typical neutron stars. They assumed the magnetic field strengths of these stars were around 3 trillion Gauss, which is in the upper range of typical neutron stars. Their simulations ran from just moments before the stars collide until just after.

What they found was that within milliseconds after the two stars make contact, the neutron fluid within the region enters a Kelvin–Helmholtz instability. This is a physics way of saying the fluid becomes turbulent. You've likely seen such an instability before. If you gently blow out a candle, there is a smooth stream of smoke that rises off the wick. But as it rises, the stream becomes swirly and random. That transition is where it reaches the instability.

The thing about Kelvin–Helmholtz instability is that it can mix things up tremendously. In the simulations, this mixes the neutron material so fully and quickly that the magnetic field is amplified significantly. This mixing trickles through the rest of the material, dragging the magnetic field with it. As a result, the resulting magnetic field of the merged neutron star can be more than 300 times stronger than the initial magnetic fields. It's also possible that further turbulence would strengthen the field even more, though this is beyond the limits of the simulation.

What's surprising about the simulation is just how quickly the magnetic field is amplified. It ripples through the stars within about a millisecond, meaning that it could play a role in how the merger progresses and could impact the structure of the resulting neutron star. More study will be needed to determine just how it plays out. But it is clear that magnetars can form through mergers like this.

Reference: Kiuchi, Kenta, et al. "A magnetar formation in binary neutron star merger." arXiv preprint arXiv:2606.11299 (2026).




By Brian Koberlein is an astrophysicist and author of the books Astrophysics Through Computation and Radio Sky: 40 Years of the Very Large Array. You can find more of his work on his website. October 20, 2026 03:34 PM UTC | Stars


Saturday, June 11, 2022

Taking the Temperature of the Solar Wind with Simulations


The sparse plasma of the solar wind fills the solar system, constantly buffets the planets, and provides the particles that generate auroras on Earth and other planets. Credit:
NASA

Researchers have applied a powerful simulation tool to a fundamental question about the solar wind: how do sparse plasmas exchange energy?


This artist’s impression of the solar wind shows a constant torrent of particles filling the heliosphere and streaming past Earth.  Credit: NASA Goddard’s Conceptual Image Lab/Greg Shirah


A Tenuous Topic

Particles bounce around equally in all directions in a substance in thermal equilibrium, but in a tenuous, magnetized plasma like the solar wind, the particles can move at very different speeds parallel and perpendicular to the magnetic field. Since temperature is a measure of the average kinetic energy of a collection of particles, this means the temperature of a plasma can be different in the direction parallel to the magnetic field lines than it is perpendicular to them!

Early plasma theory predicted that the solar wind plasma would be tens of times hotter parallel to the magnetic field than perpendicular to it. In reality, at Earth’s location, the temperature parallel to the magnetic field is, on average, just 20% hotter than the temperature perpendicular to the field lines. With few to no collisions to help the plasma come to thermal equilibrium, how is this possible?


The Kelvin–Helmholtz instability, which plays an important role in the atmospheres of stars and planets alike, is revealed by rare, wave-like patterns in clouds. Credit:
UCAR

An Unstable Solution

In a new publication, a team led by Rodrigo López (University of Santiago, Chile) used simulations to explore the impact of a plasma instability on the temperature of solar wind plasma. Plasma instabilities kick in when certain physical conditions are present, and they can have a big impact on a plasma’s large-scale characteristics, like temperature and density. While instabilities might seem abstract, they actually play a role in many common situations; weather systems, volcanic clouds, and lava lamps are all examples of instabilities at work. In each of these cases, what we observe is the result of the system spiraling away from equilibrium when it is disturbed.

Similar to these examples, instabilities can arise in a plasma in which the temperature parallel to the magnetic field is much higher than the temperature perpendicular to the magnetic field. In today’s article, López and collaborators investigated what happens to this setup when the fire hose instability comes into play. Previous work has explored the impact of the fire hose instability in plasmas where the electrons or the protons have a much higher temperature parallel than perpendicular, but relatively little work has explored what happens when both types of particles have this feature.


The change in the perpendicular to parallel temperature ratio over time for the simulated electrons (top) and protons (bottom). In Case 1, the electrons start out with a temperature ratio of 1. In Cases 2 and 3, the electron temperature ratios are 0.4 and 0.3, respectively. Credit: Adapted from López et al. 2022

Approaching Equilibrium

Using plasma physics equations and two-dimensional particle-in-cell simulations, López and coauthors found that when solar wind protons and electrons have much higher temperatures in the parallel direction, the fire hose instability takes hold of the protons much faster than it would if only the protons had this feature, while the electrons behave similarly regardless of what the protons are up to. In addition, the protons’ parallel and perpendicular temperatures draw closer when the electrons undergo the fire hose instability as well, suggesting that the electrons’ behavior is an important factor in explaining the observed temperatures in the solar wind.

Overall, the authors’ findings confirm that the fire hose instability plays an important role in moderating the temperature of the solar wind plasma, and future work should consider the influence that electrons have on the behavior of protons in the solar wind and other sparse plasmas.

Citation

“Mixing the Solar Wind Proton and Electron Scales. Theory and 2D-PIC Simulations of Firehose Instability,” R. A. López et al 2022 ApJ 930 158. doi:10.3847/1538-4357/ac66e4