Search engine for discovering works of Art, research articles, and books related to Art and Culture
ShareThis
Javascript must be enabled to continue!

Measures of correlation length at Earth’s quasi-parallel and quasi-perpendicular bow shock

View through CrossRef
Turbulent plasmas such as the solar wind and the magnetosheath exhibit an energy cascade which is present across a broad range of scales, from the stirring scale at which energy is injected, down to the smallest scales where energy is dissipated through processes such as reconnection and wave-particle interactions. Recent observations of Earth’s bow shock reveal the presence of a disordered or turbulent transition region which exhibits some features of turbulent dissipation, such as reconnecting current sheets. Understanding the variations in the origin and character of these disordered fluctuations addresses open questions such as how disordered or turbulent fluctuations in the bow shock and magnetosheath are related, and how quickly magnetosheath turbulence arises from bow shock processes. Here, we present two case studies of bow shock crossings observed by Magnetospheric Multiscale (MMS), one quasi-perpendicular and one quasi-parallel. Using high-cadence, combined search-coil and fluxgate magnetometer data, we measure changes in correlation lengths of the magnetic field through three regions: the upstream (solar wind), shock transition region, and downstream (magnetosheath). The influence of the discontinuous shock ramp is reduced using high-pass filters with variable cut-off frequencies. We find that correlation lengths are higher on the solar wind side of the shock, reducing to around 20 ion inertial lengths in the magnetosheath for both the quasi-parallel and the quasi-perpendicular shocks. We also discuss implications of the observed evolution of the correlation length to bow shock and magnetosheath processes.
Title: Measures of correlation length at Earth’s quasi-parallel and quasi-perpendicular bow shock
Description:
Turbulent plasmas such as the solar wind and the magnetosheath exhibit an energy cascade which is present across a broad range of scales, from the stirring scale at which energy is injected, down to the smallest scales where energy is dissipated through processes such as reconnection and wave-particle interactions.
Recent observations of Earth’s bow shock reveal the presence of a disordered or turbulent transition region which exhibits some features of turbulent dissipation, such as reconnecting current sheets.
Understanding the variations in the origin and character of these disordered fluctuations addresses open questions such as how disordered or turbulent fluctuations in the bow shock and magnetosheath are related, and how quickly magnetosheath turbulence arises from bow shock processes.
Here, we present two case studies of bow shock crossings observed by Magnetospheric Multiscale (MMS), one quasi-perpendicular and one quasi-parallel.
Using high-cadence, combined search-coil and fluxgate magnetometer data, we measure changes in correlation lengths of the magnetic field through three regions: the upstream (solar wind), shock transition region, and downstream (magnetosheath).
The influence of the discontinuous shock ramp is reduced using high-pass filters with variable cut-off frequencies.
We find that correlation lengths are higher on the solar wind side of the shock, reducing to around 20 ion inertial lengths in the magnetosheath for both the quasi-parallel and the quasi-perpendicular shocks.
We also discuss implications of the observed evolution of the correlation length to bow shock and magnetosheath processes.

Related Results

Energy conversion at the terrestrial bow shock
Energy conversion at the terrestrial bow shock
<p>At Earth’s bow shock, the supersonic solar wind is slowed down and deflected around the magnetosphere. To many this is "just a bow shock&...
Theia can arrive late and be oxidized, but not if it is large compared to proto-Earth
Theia can arrive late and be oxidized, but not if it is large compared to proto-Earth
The Moon-forming impact was the most significant event during the accretion of Earth substantially establishing the physical and chemical states of the Earth-Moon system. In the ca...
The Width of the Martian Bow Shock and Implications on Thermalization
The Width of the Martian Bow Shock and Implications on Thermalization
<p>In this study we have identified wide quasi-perpendicular bow shock events at Mars. We have compared these to thin quasi perpendicular bow shock events in an effor...
To bow, or not to bow
To bow, or not to bow
Name: Alexandra López Arca Main Subject: Classical Violin Research supervisor: Liesbeth Ackermans Title of Research: To bow, or not to bow. Modern bow vs. baroque bow: compariso...
Kinetic Simulations of Particle Acceleration in Collisionless Supercritical Shock-Shock Interaction
Kinetic Simulations of Particle Acceleration in Collisionless Supercritical Shock-Shock Interaction
Understanding ion energization during the interaction between an Interplanetary (IP) shock and a Bow shock remains an important and intriguing problem in space plasma physics. In t...
Archery Bow Design Equation
Archery Bow Design Equation
Bow and arrow is one of the ancient combat tool used for defense, hunting and in recent times, used in sports. There have been several improvements in archery since then. Bows, as ...
Emergence of Bow-tie Architecture in Evolving Feedforward Networks
Emergence of Bow-tie Architecture in Evolving Feedforward Networks
Abstract Bow-tie architecture is a layered network structure that has a narrow middle layer with multiple inputs and outputs. Such structures are widely seen in the...

Back to Top