B Solar Wind Particles, - reaching into Earth's magnetic field?

Click For Summary
The solar wind primarily interacts with Earth's magnetic field, resulting in most particles being deflected rather than penetrating deep into the magnetosphere. At 1 astronomical unit (AU), the solar wind's plasma flows at speeds of 250 to 750 km/s with a density of 3 to 10 particles per cubic centimeter. While some particles may reach the magnetosphere, the majority are redirected, with only a small fraction making it deeper into the magnetic field. The pressure exerted by the solar wind at this distance typically ranges from 1 to 6 nPa. Understanding these dynamics is crucial for studying the effects of solar wind on Earth's environment.
Mikael17
Messages
43
Reaction score
5
TL;DR
Solar Wind particles reaching into Earth's magnetic field ?
How many particles (approximately) from the solar wind reach deep into the Earth's magnetic field every second. Possibly measured in mass?
 
Astronomy news on Phys.org
Mikael17 said:
How many particles (approximately) from the solar wind reach deep into the Earth's magnetic field every second. Possibly measured in mass?
What do you mean by "deep"? Most of the solar wind is deflected by the Earth's magnetic field:
When the solar wind encounters Earth, it is deflected by our planet's magnetic shield, causing most of the solar wind's energetic particles to flow around and beyond us. This region that meets and blocks the solar wind is called the magnetosphere.
https://www.jpl.nasa.gov/nmp/st5/SCIENCE/solarwind.html

The Wikipedia article gives some numbers that you could use to calculate the density/flux of the solar wind near the Earth, but before it is deflected by the magnetospnere:
Velocity and density

Near the Earth's orbit at 1 astronomical unit (AU) the plasma flows at speeds ranging from 250 to 750 km/s with a density ranging between 3 and 10 particles per cubic centimeter and temperature ranging from 104 to 106 Kelvin.[45]

On average, the plasma density decreases with the square of the distance from the Sun, see Section 4.2,[46] while the velocity decreases and flattens out at 1 AU, see Figure 5.[46]

Voyager 1 and Voyager 2 reported plasma density n between 0.001 and 0.005 particles/cm3 at distances of 80 to 120 AU, increasing rapidy beyond 120 AU at Heliopause to between 0.05 and 0.2 particles/cm3.[47]

Pressure

At 1 AU, the wind exerts a pressure typically in the range of 1–6 nPa ((1–6)×10−9 N/m2),[48] although it can readily vary outside that range.

The ram pressure is a function of wind speed and density. The formula is

P = m p ⋅ n ⋅ V 2 = 1.6726 × 10 − 27 k g ⋅ n ⋅ V 2 {\displaystyle P=m_{\text{p}}\cdot n\cdot V^{2}=\mathrm {1.6726\times 10^{-27}\,kg} \cdot n\cdot V^{2}}

where mp is the proton mass, pressure P is in Pa (pascals), n is the density in particles/cm3 and V is the speed in km/s of the solar wind.[49]
https://en.wikipedia.org/wiki/Solar_wind
 
  • Like
Likes Delta Prime
Some 8 years ago I posted some experiments using 2 Software Defined Radios slaved to a common clock. The idea was measure small thermal noise by making correlation measurements between the IQ samples from each radio. This is a project that has kinda smoldered in the background where I've made progress in fits and starts. Since most (all?) RA signals are small thermal signals it seemed like the technique should be a natural approach. A recent thread discussing the feasibility of using SDRs to...