Solar Storm Threat Analysis - Impact
Solar Storm Threat Analysis - Impact
Solar Storm Threat Analysis - Impact
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<strong>Impact</strong>, 2007 James A. Marusek<br />
The severity of a geomagnetic storm depends on the orientation of Earth's magnetic field in relation to the solar<br />
storm magnetic orientation. If the particle cloud has a southward directed magnetic field it will be severe, while if<br />
northward the effects are minimized.<br />
A CME can produce the following affects: electrostatic spacecraft charging, shifting of the Van Allen radiation belt,<br />
spacetrack errors, launch trajectory errors, spacecraft payload deployment problems, surveillance radar errors, radio<br />
propagation anomalies, compass alignment errors, electrical power blackouts, oil and gas pipeline corrosion,<br />
communication landline & equipment damage, electrical shock hazard, electrical fires, heart attacks, strokes, and<br />
workplace & traffic accidents.<br />
B. Scope of <strong>Solar</strong> <strong>Storm</strong> <strong>Threat</strong><br />
Great solar storms occur approximately once per decade. Table 4 lists the great solar storms over the past 150 years.<br />
The largest solar storm ever recorded occurred on 1-2 September 1859. It was the greatest solar storm in the past<br />
450 years. But this still leaves open the question. Could our sun produce an even greater solar storms than the one<br />
observed in September 1859?<br />
.<br />
Date <strong>Solar</strong> Flare<br />
Intensity<br />
1-2 September 1859 Sept 1 Carrington<br />
White Light Flare [2]<br />
Table 4. Great <strong>Solar</strong> <strong>Storm</strong>s<br />
Omni-Directional<br />
<strong>Solar</strong> Proton<br />
Fluence<br />
4<br />
Main CME<br />
Arrival Time<br />
1.88 x 10 10 cm -2 [8] 17 hours<br />
40 minutes [9]<br />
Magnetic Intensity<br />
Disturbance <strong>Storm</strong> Time<br />
(Dst) (nano-Teslas)<br />
Sept 2 - 1,760 nT [9]<br />
(∆H at Bombay 1,720 nT)<br />
12 October 1859 (∆H at Bombay 980 nT) [9]<br />
4 February 1872 (∆H at Bombay 1,020 nT) [9]<br />
17-18 November 1882 (∆H at Greenwich > 1,090 nT) [9]<br />
30 March 1894 1.11 x 10 10 cm -2 [8]<br />
31 October 1903 (∆H at Potsdam > 950 nT) [9]<br />
25 September 1909 (∆H at Potsdam > 1,500 nT) [9]<br />
13-16 May 1921 (∆H at Potsdam 1,060 nT) [9]<br />
7 July 1928 (∆H at Alibag 780 nT) [9]<br />
16 April 1938 (∆H at Potsdam 1,900 nT) [9]<br />
13 September 1957 Sept 13 - 427 nT [10]<br />
11 February 1958 Feb 11 - 426 nT [10]<br />
13 March 1989 X15 Mar 13/14 - 589 nT [10]<br />
29 October -<br />
5 November 2003<br />
Oct 28 X17.2<br />
Oct 29 X10<br />
Nov 4 X45 [11]<br />
19 hours Oct 29 -353 nT [10]<br />
Oct 30 -383 nT [10]<br />
Nov 5 (missed Earth)<br />
18-21 November 2003 Nov 18 M3.2 [9] Nov 20/21 - 422 nT [10]<br />
Dst is an abbreviation for the Disturbance <strong>Storm</strong> Time index that measures the strength of the magnetic storm by<br />
averaging the horizontal components of the geomagnetic field.<br />
M-type dwarf stars called “flare stars” have been observed to create massive solar flares that can outshine their stars<br />
by over 1000 times. A two star system called “II Pegasi” produced a stellar flare in 2006 on a scale previously<br />
unimaginable for anything other than a supernova. The flare was a hundred million times more energetic than the<br />
sun’s typical solar flare, releasing the equivalent energy of 50 million trillion nuclear bombs. A solar “superflare”<br />
would cause significant death & destruction to Earth if it was directed towards our planet. But our sun doesn’t fit<br />
these conditions. Our sun is a G-type star. Nor does our sun have a companion star revolving extremely close<br />
around it at distance of only a few stellar radii.