Plasma density contours from a 3D magnetohydrodynamic model of the
heliosphere. The interstellar plasma (orange) increases in density at the
bow shock (red). The lower density (blue) solar wind plasma increases in
density at the termination shock (blue-turquoise interface). Charge exchange
processes involving shock-heated solar wind ions produce energetic neutral
atoms that can be imaged to provide information on the 3D structure of the
termination shock. Higher energy neutral atoms resulting from the
charge-exchange of anomalous cosmic rays with interstellar hydrogen can also
be imaged. Shock accelerated particles are ubiquitous in the universe and
the termination shock provides a unique opportunity to study the detailed
properties of a large-scale shock, in situ, including its effect on the
plasma, magnetic fields, and energetic particles that encounter it.
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- What is the size and structure of the heliosphere?
- How do the termination shock and heliopause respond to solar variations and interstellar pressure?
- How does the interstellar medium effect the inner heliosphere and solar wind dynamics?
- What roles do thermal plasma, pickup ions, waves, and anomalous cosmic rays play in determining the
structure of the termination shock?
- What are the properties of interstellar gas and dust that penetrate into the heliosphere?
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