Notes On EMP And Its Effects
Source: Federation of American Scientists
May 20, 1999
Jon Bell’s question about EMP and its effect
"As I understand them, EMP weapons have a radius of
coverage of about 25 to 50 miles from their detonation point
(still quite a problem). Does anyone know if Lukin’s statement that
the EMP from a nuclear weapon detonated at high altitude
could affect the entire U.S. is true? "
An "EMP weapon" is not the same as a large nuclear
explosion that is detonated at high altitude with the damage range
over 1000 km. http://www.fas.org/nuke/hew/Library/Damage
My source of information comes from a paper by Carey
Sublette of the Federation of American Scientists
(www.fas.org) and their nuclear weapon section at:
http://www.fas.org/nuke/hew/index.html
Allow this gentleman to explain the science:
http://www.fas.org/nuke/hew/Nwfaq/Nfaq5.html#nfaq5.4
(Begin excerpt....)
5.5 Electromagnetic Effects (of nuclear weapons)
The
high temperatures and energetic radiation produced by
nuclear explosions also produce large amounts of ionized (electrically
charged) matter which is present immediately after the explosion.
Under the right conditions, intense currents and electromagnetic
fields can be produced, generically called EMP (Electromagnetic
Pulse), that are felt at long distances. Living organisms are
impervious to these effects, but electrical and electronic equipment
can be temporarily or permanently disabled by them. Ionized gases can
also block short wavelength radio and radar signals (fireball
blackout) for extended periods.
The occurrence of EMP is strongly dependent on the
altitude of burst. It can be significant for surface or low
altitude bursts (below 4,000 m); it is very significant for high
altitude bursts (above 30,000 m); but it is not significant for
altitudes between these extremes. This is because EMP is generated by
the asymmetric absorption of instantaneous gamma rays produced by the
explosion. At intermediate altitudes the air absorbs these rays fairly
uniformly and does not generate long range electromagnetic
disturbances.
The formation EMP begins with the very intense, but
very short burst of gamma rays caused by the nuclear reactions
in the bomb. About 0.3% of the bomb’s energy is in this pulse, but it
lasts for only 10 nanoseconds or so. These gamma rays collide with
electrons in air molecules, and eject the electrons at high energies
through a process called Compton scattering. These energetic electrons
in turn knock other electrons loose, and create a cascade effect that
produces some 30,000 electrons for every original gamma ray.
In low altitude explosions the electrons, being very
light, move much more quickly than the ionized atoms they are removed
from and diffuse away from the region where they are formed. This
creates a very strong electric field which peaks in intensity at 10
nanoseconds. The gamma rays emitted downward however are absorbed by
the ground which prevents charge separation from occurring. This
creates a very strong vertical electric current which generates
intense electromagnetic emissions over a wide frequency range (up to
100 MHZ) that emanate mostly horizontally. At the same time, the earth
acts as a conductor allowing the electrons to flow back toward the
burst point where the positive ions are concentrated. This produces a
strong magnetic field along the ground. Although only about 3x10^-10
of the total explosion energy is radiated as EMP in a ground burst
(10^6 joules for 1 Mt bomb), it is concentrated in a very short pulse.
The charge separation persists for only a few tens of microseconds,
making the emission power some 100 gigawatts. The field strengths for
ground bursts are high only
in the immediate vicinity of the explosion. For smaller bombs they
aren’t very important because they are strong only where the
destruction is intense anyway. With increasing yields, they reach
farther from the zone of intense destruction. With a 1 Mt bomb, they
remain significant out to the 2 psi overpressure zone (5
miles).
High altitude explosions produce EMPs that are
dramatically more destructive. About 3x10^-5 of the bomb’s total
energy goes into EMP in this case, 10^11 joules for a 1 Mt bomb. EMP
is formed in high altitude explosions when the downwardly directed
gamma rays encounter denser layers of air below. A pancake shaped
ionization region is formed below the bomb. The zone can extend all
the way to the horizon, to 2500 km for an explosion at an altitude of
500 km. The ionization zone is up to 80 km thick at the center. The
Earth’s magnetic field causes the electrons in this layer to spiral as
they travel, creating a powerful downward directed electromagnetic
pulse lasting a few microseconds. A strong vertical electrical field
(20-50 KV/m) is also generated between the Earth’s surface and the
ionized layer, this field lasts for several minutes until the
electrons are recaptured by the air. Although the peak EMP field
strengths from high altitude bursts are only 1-10% as intense as the
peak ground burst fields, they are nearly constant over the entire
Earth’s surface under the ionized region.
The effects of these field on electronics is
difficult to predict, but can be profound. Enormous induced electric
currents are generated in wires, antennas, and metal objects (like
missiles, airplanes, and building frames). Commercial electrical grids
are immense EMP antennas and would be subjected to voltage surges far
exceeding those created by lightning, and over vastly greater areas.
Modern VLSI chips are extremely sensitive to voltage surges, and would
be burned out by even small leakage currents. Military equipment is
generally designed to be resistant to EMP, but realistic tests are
very difficult to perform and EMP protection rests on attention to
detail. Minor changes in design, incorrect maintenance
procedures, poorly fitting parts, loose debris, moisture, and ordinary
dirt can all cause elaborate EMP protections to be totally
circumvented. It can be expected that a single high yield, high
altitude explosion over an industrialized area would cause massive
disruption for an indeterminable period, and would cause huge economic
damages (all those damaged chips add up).
A separate effect is the ability of the ionized
fireball to block radio and radar signals. Like EMP, this effect
becomes important with high altitude bursts. Fireball blackout can
cause radar to be blocked for tens of seconds to minutes over an area
tens of kilometers across. High frequency radio can be disrupted over
hundreds to thousands of kilometers for minutes to hours depending on
exact conditions.
by Carey Sublette
http://www.fas.org