Radiation and the Van Allen Belt

The Particles in the Van Allen Belt

Server Sky arrays in the initial m288 orbit are in the "slot" between the inner and outer Van Allen belts. The radiation is somewhat lower, but still very high. The main difference between the belts is the mechanisms creating them.

The inner belt is mostly created by C.R.A.N.D. - Cosmic Ray Associated Neutron Decay. Cosmic rays striking the upper atmosphere split atoms and generate neutrons with energies above 30MeV. Unbound neutrons have a half-life of 10 minutes and move at more than 10% of the speed of light. The neutrons undergo beta decay and split into an electron, a proton, and an electron antineutrino. 10 minutes at 0.1c is about 20 million kilometers, about 50 times the diameter of the moon's orbit, depositing the particles mostly in that huge volume. The density of these deposited particles falls off as 1/R2, so the highest density of these decays occur near the Earth. The electron gets most of the 2MeV beta decay energy, but the proton retains most of the original momentum and energy of the neutron, and have about the same average energy and direction as the original neutron. The electrons are much less massive, so the 2MeV makes them move faster, approaching the speed of light. If the neutron decay occurs in the Earth's magnetic field, and most of the momentum is perpendicular to, rather than parallel to, the magnetic field lines, then the proton spirals around the field lines and gets captured in the Van Allen belt. The likelihood of any neutron decaying within the Van Allen Belt is small - but that small probability is larger in the inner belt, closer to the source.

The outer belt is mostly composed of protons and electrons captured from the solar wind, but does include some helium and larger nuclei. In solar storms (flares and coronal mass ejections), the earth's magnetic field is hammered and some of these particles migrate inwards, and a few are pumped up to higher energy.

Once captured by the magnetic field in either belt, charged particles gyrate around the lines of magnetic field from the earth - cyclotron resonance. A 10 MeV proton has a gyroradius of approximately 700 km at 6400 kilometers altitude. Particles have some velocity parallel to the field lines, and travel up and down the field lines as they circle helically around them. The field strength increases as it gets closer to the earth, and this causes the particles to lose perpendicular velocity, then bounce back the other way, at the "mirror point". If the ratio of the parallel velocity to the perpendicular velocity is high enough, the particles will collide with the upper atmosphere before they reach their mirror point, and are taken out of circulation. So only a tiny fraction of source particles become captured electrons and protons, and only a small fraction of those do not collide with the atmosphere.

Of the few particles that do get captured, and "survive infancy", most remain in the belts for a long time, some for thousands of years, until they scatter off other particles and increase their ratio of parallel to perpendicular velocity, then drop into the atmosphere. So the generation rates are small, and the recombination rates are small also.

The total mass of particles in the entire Van Allen belt is on the order of 10 grams. However, the particles are moving very fast and store a lot of energy. Any object in orbit will be hit by only a tiny fraction of them, but the particles that do hit an object may deposit a lot of energy and cause a lot of damage, especially to semiconductor lattices and long-chain organic molecules.

Earth's Magnetic Field

Without a magnetic field, nothing would hold these high energy charged particles near the Earth - they would rapidly dissipate into empty space. So, understanding the magnetic field is essential to understanding how the charged particles move.

The Earth's magnetic field is complicated, but to first order, the field can be approximately modeled as a "dipole", similar to a bar magnet with a north and south pole. The dipole is not conveniently placed at the center of the earth, and is not lined up with the rotation axis. It is displaced more than 500km north and outwards from the center of the earth, and is tilted about 11 degrees with respect to that center. The center and direction change over time, causing the north and south magnetic poles to drift about 40 kilometers a year, on random looping trajectories. In 2005, the dipole center was located 552 kilometers from the Earth's center, 22.2 degrees north of the equator (209 kilometers) and 511 kilometers radially outwards from the rotation axis, in the direction of 141.6 east longitude. This spot is between the center of the earth and a point on the Pacific ocean about halfway between Japan and Guam.

The 2006 dipole was tilted by 10.26 degrees from north-south, and further rotated into a plane that is 71.78 degrees west of the prime meridian. This shifts the North geomagnetic pole (the place where the dipole axis surfaces to the north) among the islands north of Canada. The south geomagnetic pole is in Wilkes Land, near the coast of Antarctica and south of Western Australia. The magnetic poles, where the field lines are on average vertical to the earth's surface, are in two other locations.

In space, we are not concerned with the poles, or the surface fields, but in the paths of the field lines as they leave the earth's surface in the north and reenter the surface in the south. The field lines follow a path where the radial distance r from the center of the earth is defined by r = L R_e \sin( \phi )^2 . \phi is the angle from the magnetic dipole axis, so the radial distance is zero in the direction of the north and south magnetic poles, and maximum in the magnetic equatorial plane (which is tilted and displaced from the plane defined by the earth's rotation). R_e is the earth's radius (6378km at the equator) and L is the McIlwain L-parameter. All the field lines with the same L parameter form a flattened and somewhat distorted torus, called an L-shell. The L=1 shell is mostly within the earth, bulging outwards above the earth over the Pacific, while staying below the surface elsewhere. The L=2 shell extends to 2x6378 or 12756 kilometers from the center of the dipole. Since the dipole is offset by about 400 kilometers, the altitude of the L=2 shell magnetic equator varies between about 5900 and 6900 kilometers above the surface of the earth.

The L=1.1 shell and the L=2.0 shells are illustrated in the following animation:

Embedded application/x-shockwave-flash

magf05.pov povray source . . . magf05.ini povray control file . . . povinc.tar.gz povray include files

Notice how the 1.1 shell comes very close to the surface over Brazil and the south Atlantic. This causes the South Atlantic Anomaly, where the bottom of the Van Allen Belt comes very close to the surface and low earth orbits get a lot of radiation. The red "poles" indicate the north and south rotational poles, the yellow poles indicate the axis of the inner dipole. The north end of the dipole is tilted towards Canada, and center of the dipole is displaced radially towards Japan.

The server sky orbit is equatorial, elliptical with a semimajor axis of 12789km and an eccentricity of 0.0226 (to avoid Lageos). The perigee radius is 12502km and the apogee radius is 13080km. The magnetic field is offset compared to the orbit. Over an orbit, the L shell varies like so:

L shell versus orbit angle

ll288a.c c source . . . XXXXX3.gp gnuplot commands

Arrays experience slightly different radiation conditions at different parts of their orbit. The orbit "dwells" in the upper and lower L shell extremes when these correspond with apogee (local midnight) or perigee (local noon). These extremes occur at 125° west, over the western United States, and western Europe at 0°. Since diffusion between L shells, and magnetic storm distortion, is likely to inject particles at these extremes, these will tend to be higher radiation error regions, requiring more recomputes, and resulting in slower throughput.

Fortunately, these regions of the world are already well served by existing compute and fiber optic infrastructure. New and unserved markets in Asia and the western Pacific, from 40° to 150%deg; east, will be in the lowest error regions. Those parts of Asia will be the biggest early market opportunities, By the time Europe, the Western US, and Africa are ready for maximum extra communication and computation, the constellations will be thick enough to Rutherford-scatter all the intersecting L shells, and designs will evolve towards more radiation error resistance and a lower longitude penalty.

MoreLater - I need to check my work, the shell animation seems to show the "top bulge" (corresponding to minimum L shell) over Asia. Hmmm --- there goes the business plan. :-(

Radiation Dose in 35 micrometer thick aluminum

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Rutherford Scattering by Millions of Thinsats

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Radiation (last edited 2016-02-05 03:36:59 by KeithLofstrom)