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Making Deep Space and Nuclear
Rockets Safe for Astronauts: PART I
As
far back in human history as one would care to go the exposure to
radiation has always existed with Homo Sapiens thus the need to protect
people whose occupation requires them to work or travel among natural or
man-made excessive sources of ionizing radiation anywhere in the Solar
System.
It was only in the later part of the 19th century that
scientists found the existence of accelerated particles as cathode rays
by Geissler and Pluecker in 1859 these were later extracted as an
external beam by Lenard in 1893. Roentgen would repeat Lenard's
experiments and discovered more diffuse penetrating x-rays produced at
the fluorescent impact site of a cathode rays on the tube wall or
external target.
This began a history of subatomic particle use in service to medical
diagnostic and therapeutic tools. In those early days x-ray penetrating
power came with a price as in misuse and reports of adverse biological
effects like dermatitis, sore eyes and hair falling out followed by
reports of cancer within an x-ray produced ulcer and other adverse
biological consequences. It wasn't till Becquerel in 1896 that he
convinced the scientific community of his day that these same x-rays
were inherent properties of the uranium atom. Rutherford discovered two
radioactivity rays as alpha and beta of different penetrating power as
emissions from uranium Becquerel showed that Rutherford's beta ray was
the same as cathode rays. The Curies discovered that uranium ores
contain other radioactive elements as radium and polonium. If the
radioactive decay times of 235U, 238U and 232Th
(and to a lesser extent 87Rb and 40K) were not on
the order of the age of the universe, there would be no significant
natural radioactivity, the development of nuclear physics would have
been delayed for decades, and nuclear energy based on fission would not
have developed 1.It was their mental and
physical sacrifice that led them to win the first of the Noble prizes
and the beginnings of an atomic age.
Along with this novus technology came the understanding that these
"Rays" cause ions to be generated in the air and other matter enhancing
the conduction of electrical charge and producing chemical change. It
was also known that ions present in the atmosphere could discharge
condensers (electrometers/electroscopes)
over a period of time and the rate of increased discharge was caused by
these known radioactivity rays: cathode rays, x -rays.
Brief History
of Ambient Radiation Detectives
By 1901, research
into natural radioactivity had discovered three particles capable of
causing ionization of air and discharging electroscopes. In 1910, Thomas
Wulf S. J., climbed to the top of the Eiffel Tower and showed that the
ionization was not due to fl-rays from the earth 2.
Wulf rightly concluded that radiations must be penetrating from the top
of the atmosphere, although that interpretation was controversial.
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Victor Hess Launching Balloon 1912 |
Between 1912-1913 V.F. Hess
developed electrometer experiments by carrying them aloft in a balloon
he found that radiation did indeed arrive from the top of the Earth's
atmosphere His studies found ionization rates to decrease with altitude
up to 500m followed by a steady increase at higher altitudes to where
the ground level rate is matched at 1,500m.
For this discovery he received a Noble
prize in physics in 1936. The term 'cosmic radiation' came into being in
1926.
Another important contributor to
the understanding of natural charge particles was the term 'cosmic ray'
was coined by Robert Millikan in 1925.
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Robert A. Millikan
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The discovery of his law of
motion of a particle falling towards the earth after entering the
earth's atmosphere, together with his other investigations on electrical
phenomena, ultimately led him to his significant studies of cosmic
radiation (particularly with ionization chambers). The last piece of
important evidence from a human exposure perspective was the discovery
of heavy ion tracks by
Phyllis Frier
and co-workers using nuclear emulsion track detectors in high-altitude
balloon flights. Although the initial emphasis of this discovery was the
ability to sample cosmic matter, attention would turn to the possibility
of human exposure by these ions in high-altitude aircraft and future
space travel.3 The trapped radiation were
directly observed by the first United States satellite launched in 1958
with a Geiger-Mueller tube.
BASIC CONCEPTS
Human activity has
increased human exposures to natural radiation because of technological
development.
The concept of field
refers to the spatial distribution of a physical quantity which may vary
with time of observation. Ionizing radiation refers to the field
associated with a physical agent which has the property of producing
ions within a material substance placed within the field.
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Dr. William H. Pickering, former
director of JPL, which built and operated the satellite. Dr.
James A. van Allen, center, of the State University of Iowa,
designed and built the instrument on Explorer that discovered
the radiation belts which circle the Earth. At right is Dr.
Wernher von Braun, leader of the Army's Redstone Arsenal team
which built the first stage Redstone rocket that launched
Explorer 1. NASA PHOTO
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The ionizing
radiation field itself consists of particles streaming from some source
and could be either charged or neutral particles. The ionization within
substances is ultimately associated with the transfer of kinetic energy
of the field particles to bound electrons of the substance by which
molecular changes are initiated. In the case of charged particle fields
(electrons, muons, pions, protons, alpha particles, and other ions), the
ionization is caused directly through coulombic interaction between the
radiation field constituents and bound electrons in the substance. In
the case of neutral particle fields (photons and neutrons), the
ionization is mainly indirect by the release of an energetic charged
particle within the substance. Ionization induced by photons is mainly
the result of transfer of photon energy to a bound electron providing
sufficient kinetic energy to the electron resulting in additional
ionizing events. Ionization induced by neutrons is through a nuclear
collision event in which a recoiling nucleus or energetic charged
nuclear reaction products are the agents of ionization. The ionization
process in living tissues consists of ejecting bound electrons from the
cellular molecules leaving behind chemically active molecular species
(radicals) which are the source of adverse changes. Cellular processes
are able to overcome most of this injury as many of the radicals
resulting from radiation injury are similar to those produced in
ordinary metabolic processes for which the cell has developed recovery
mechanisms needed for long term survival (Billen 1990)4.

Conventional wisdom considers changes in the DNA structure as the
substantive target of radiation injury which may also be injured
directly by the passing ionizing particle. The ability of the cell to
repair the effects of ionization depends in part on the number of such
events occurring within the cell from the passage of a single particle
and the rate at which such passages occur. The number of ionization
events per particle passage is related to the physical processes by
which particle kinetic energy is transferred to the cellular bound
electrons. Charged particles have a long range interaction and tend to
loose energy through small discrete events over short mean free paths on
the order of atomic dimensions and appears as a continuous slowing down
process similar to motion of an object through a viscous media. The rate
of energy loss increases rapidly with increasing charge of the particle
and decreasing speed. The rate of energy loss of electrons and singly
charged ions at high energies are more like photon exposures in their
biological consequences. The distance traveled depends on the inertia
and massive particles are more penetrating than lighter particles of the
same charge and speed. Uncharged particles have longer free paths and
for neutrons larger energy transfers per event resulting in energy
losses which appear as isolated occurrences along the particle’s path.
The electrons resulting from photon interactions produce few ions in
isolated cells and the rate at which such events occur in a given cell
is important since repair of a single event is relatively efficient
unless many events occur within the repair period (Wilson et al. 1993).
Indeed, the single photon event may do little more than add a few free
radicals to the melee of metabolic related radicals and have little or
no added consequence (Billen 1990). The effects on health risks of dose
rate of the exposures is included in protection through a Dose Rate
Effectiveness Factor DREF. The massive low energy ions resulting from
neutron interactions always produce copious ions in the struck cell and
repair is less efficient for such events. Unlike photon doses which are
ineffective in causing injury unless many interactions occur within the
cell’s repair period (i.e., high dose rates), neutron exposures under
most conditions will be singular events in a few cells and will not be
so dependent on the dose rate as is true for high LET radiation events
of heavy ions (Schaefer 1952, Curtis et al. 1995, Wilson et al. 1995a).5
Allowable exposures
depend on the radiation risk coefficient, an assessment of acceptable
risk levels, the exposed individual’s knowledge of the exposure, and
relationship to the individual’s possible benefit as related to the
exposure. For example, exposure of the general public is kept low since
they may not even be aware of the exposure and may not directly benefit.
Such public exposures are limited to be on the order of natural
background levels (ICRP 1991). Those occupationally exposed derive a
direct benefit from their work activity and are informed of their
exposures. Occupational exposure levels are limited to risk levels
comparable to risk of accidental death in moderately safe industries.
Astronaut annual exposures may be quite high since they are informed,
receive benefit from their occupation, start careers in mid-life, and
are limited to a short career duration so that their lifetime risks are
comparable to career lifetime risks of death in moderately safe
industries.
Pregnancy
is a separate issue since the exposed individual is highly sensitive,
receives no direct benefit, and is allowed to be exposed by decision of
the parent. The current regulatory limits and proposed new limits are
shown in table 1.6
Terrestrial Background Exposures
The term
terrestrial background exposure is used here in the sense that these
exposures are the normal result of everyday living in our present
culture. Primordial matter consists of a vast array of elemental
components, many of which were unstable to radioactive decay and have
long since disappeared in the 4.5 billion years of earthly existence.
Only those primordial
elements with unusually long decay times (U-238, Th-232, U- 235, Rb-87,
and K-40) remain within the Earth's crust (Halliday 1962). These are the
principal sources of exposure on the Earth's surface. There are three
main decay chains headed by the long lived isotopes U-238, Th-232, and
U-235 which decay by sequential emission of alpha,
beta, and gamma rays. The rates of decay within
these chains are dominated by the lifetime of the longest lived isotopes
at the head of the chain. A fourth decay chain Np-237 exists but was of
sufficiently short decay time to have since disappeared from the Earth’s
environment.
The emitted particles are in order of increasing range in matter as
alphatens of micrometers, beta-few centimeters, and gamma-many meters.
Unless internalized, only the gamma rays are of consequence in human
exposures. A detailed summary of terrestrial exposures is given in NCRP
Report 93 (1987).
Among the decay products of these radioactive chains is the noble gas
radon which can become airborne and inhaled (along with its airborne
decay products) resulting in exposures of lung tissues. Rn-222 produced
in the U-238 decay sequence is the main source of such exposures
although Rn-220 from the Th-232 sequence makes non-negligible
contributions. Radon related exposures are mainly through alpha emission
and the bronchial epithelium is primarily exposed. Even then the main
exposures result from breathing the trapped air within buildings and
depends on location and construction techniques. The US average annual
radon decay effective dose equivalent to lung tissues is given in table
3 as 2 mSv and consists of high LET alpha particles with an assumed
quality factor of 20 (Q=20).
Terrestrial Occupational Exposures
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Typical exposure of any individual within the US population from the
several background sources in table 3 are within a factor of two of the
average values shown. In addition to these exposures, there are those
whose work activity result in an occupational radiation hazard. The
number of individuals for whom occupational exposures are part of the
workday have increased dramatically with developing technology from
216,000 in 1958 to 1.1 million in 1975 to an estimated 1.3 million in
1980. The estimated average exposure for this class of people had
declined from 2.4 mSv to 1.1 mSv over the same period. Typically half of
the identified radiation workers had only negligible exposures so that
the average of those with significant exposures was 4.8 mSv in 1958
dropping to 2.2 mSv in 1980. The remainder of the radiation workers
experienced only (or nearly) background levels as typified by table 3.
Note that the average occupational effective dose equivalent is on the
order of the background levels in table 3. Even so there are a few
radiation workers who are near maximal exposure levels in table 1 but
have only small impact on averages due to their small number. Most
individual radiation worker exposures in 1980 are within a factor two of
the 2.2 mSv.7
Past Commercial Air Transportation Studies
When
the possibility of high-altitude supersonic commercial aviation was
first seriously proposed, Foelsche brought to light a number of concerns
for the associated atmospheric radiation exposure due to penetrating
cosmic rays (CR) from the galaxy (GCR) and the sun (SCR also referred to
as solar particle events, SPE) including the secondary radiations
produced in collision with air nuclei (Foelsche 1961, Foelsche and Graul
1962). Subsequently, a detailed study of the atmospheric ionizing
radiation components at high altitudes was conducted from 1965 to 1971
at the Langley Research Center (LaRC) by Foelsche et al. (1974 ).8
Space Exposure Limits
The
Earth’s protective atmosphere is a massive 1 kg/cm2 or equivalent mass
of ten meters of water. There is little wonder that the cosmic ray
levels are low on the surface and still modest at aircraft altitudes
where only 25 percent of the atmosphere remains to protect subsonic
aircraft and only 5 percent remains to shield the HSCT. Even so, 5
percent is equivalent to 50 cm of water. Even if one is above the
atmosphere, there is still the geomagnetic field which provides
protection from extraterrestrial radiations near the equator (low
inclination orbits) but also poses a new hazard from those particles
trapped in the geomagnetic field itself (see figure 2). In addition to
the greater intensities of the space radiation environment, the
astronaut is committed to 24 hours of exposure time for each work day
unlike any other occupational exposure. For these reasons, astronaut
exposure limits have always been considered outside the realm of other
radiation related occupations.9
Deep Space Mission
Exposures
Outside
the geomagnetosphere, astronauts are subject to the full galactic and
solar cosmic ray environments except for what protection is afforded by
the vehicle or spacesuit. The GCR are of low intensity and were not of
concern in the Apollo mission which were of short duration (less than
two weeks). The main concern was the possibility of a solar particle
event in which acute effects may occur as was reflected in the design
exposure limits in table 6. As future space exploration is towards Mars
and there is the possibility of a lunar colony, the long term exposures
to galactic cosmic rays are a critical issue (NCRP 1989).
There are no exposure standards for such missions established since the
biological cancer risks and other adverse effects of exposures to the
HZE ions are largely unknown (NAS 1996). Galactic background exposures:
The galactic cosmic rays are more intense outside the solar system and
must overcome the outward convection of the solar wind. As the solar
wind changes intensity over the changing solar cycle (see sunspot
numbers in figure 11) there is a corresponding inverse variation in
cosmic ray intensity within the solar system. The solar modulation zone
extends to 100 astronomical units but intensities vary only slightly
between Earth and Mars (about 10 percent or less, Fujii and McDonald
1997).10
Concluding Remarks
Exposures
in low Earth orbit with low inclination have a large contribution from
low LET components for which the risk coefficient is relatively well
defined. The reverse is true for high inclination where a significant
fraction of the exposure is from HZE ions (table 14). Even the shield
design based on dose equivalent as in the case of the International
Space Station may be misleading with respect to control of the health
risk.
Deep space mission
exposures from background are dominated by HZE ions and the
corresponding risk uncertainties are large (NAS 1996). Traditional
construction materials like aluminum probably increase the health risks
but polymeric materials show some usefulness in shielding the astronaut
from the HZE ions.
Solar particle event (SPE) exposures in LEO are limited by the natural
precessional motion of the spacecraft even in the event of a concurrent
large geomagnetic storm. Crew rotation may be required after such an
event but health risks are manageable. In deep space, solar events can
present a serious health hazard and adequate monitoring with a warning
system and storm shelter design is required. Large exposures are
possible if adequate shelter is not acquired in a timely fashion. Still
lethality is not likely since tissue repair greatly reduces the effect
of exposure and especially if adequate medical planning is part of the
mission design. Space stress could greatly alter the biological response
to such exposures and an adequate understanding of space stress affects
is necessary to mission planning.11
Shielding Humans in Deep Space
In
1995 a workshop was conducted by NASA, DOE Lawrence Berkeley Laboratory,
NOAA Space Environmental Laboratory, the National Academy of Science
Space Studies Board, aerospace industries and several universities to
tailor strategies with regard to shielding humans required to live and
work on lunar and martian environments from hazardous levels of
radiation.12
The
workshop's object was to devise strategies to conduct missions to reduce
the levels of radiation to as low as reasonably achievable so that
astronauts could conduct safely their missions and return to conduct
future missions. The radiation exposure risks health risks to the
astronaut had to be kept at acceptable levels currently taken at :
- Not more than
3% lifetime excess fatal cancer risks.
- Prevention of
radiation sickness which may impact mission safety (lethality,
vomiting, nausea etc.).
This
workshop dealt with manipulation of lunar and martian regolith to
provide the least most efficient expenditure of cost and energy to
conduct base operations. Habitats were designed, vehicles and soil
moving equipment were examined space suits were evaluated, solar event
early warning system, radiation shielding material and design issues
were assessed to find the best method to protect human and
microelectronics from the effects of dangerous space radiation.
Candidate shielding materials like:
- Lunar
Regolith 56% SiO2 | 19.8% FeO | 17.5%W% Al2O3 | 10% MgO | density
0.8-2.15g/cm2*
- Martian
Regolith 58.2% SiO2 | 23.7% FeO2O3 | 10.8%MgO | 7.3%CaO | density
1.0-1.8g/cm2
- Aluminum
- water
- Lithium
hydride
- Magnesium
hydride (good medium because its use as a hydrogen storage medium
(non cryogenically)
- Polyethylene
- Borated
polyethylene
-
Regolith/epoxy
- Epoxy
-
Polyetherimide
- Polyamide
- Polysulfone
-
Polytetrafluoroethylene
- Hydrogen
* studies show
lunar regolith at 75g/cm2 of regolith will reduce the annual GCR dose
solar event minimum/large flares to LEO limit operation limits.
As the study
pointed out the need to provide a comfortable margin of radiation
mitigation is the goal since transporting around sick or dying
astronauts isn't good human exploratory space policy - as the saying
goes, "Better safe than sorry."
SPACE RADIATION BUSTERS
*FEATURE INTERVIEW*
INTERVIEW WITH JOHN W. WILSON
RADIATION SHIELDING AND MITIGATION STUDIES
LANGLEY RESEARCH CENTER NASA
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Dr. John Wilson and his wife of 40 years
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Hello ...I'm Bruce Behrhorst writer for the online publication
nuclearspace.com...
I would like to thank you, Dr. John W. Wilson for volunteering your time
to speak with us this October 2003 day.
I understand that you have been involved with Dr.
Frank Cucinotta in Space Radiation Health Risk Mitigation Technologies
at Langley NASA for a number of years is that correct.?
JW:
We started back in the mid eighties working together for I guess twenty
years now that we've been working this problem.
BB:
Could you explain your office?
JW:
The main thing that we do at Langley is to look at the development of
computational procedure for estimation of cancer risk within various
material configurations and seeking what materials give the optimum
amount of protection to the astronaut. And in particular we look for
materials that we can use in some sort of multifunctional mode so that
we don't think of shielding so much as adding something into a design
that's already been pretty well established. Actually integrating good
materials in the overall design as a way to try and optimize the
spacecraft. So primarily the focus we have here and Frank [Cucinotta]
was part of this group up until about 1990-91 more like ' 95 and we had
begun a process looking at biological models he at Langley trying to
understand what the impact of the biological models were on the shield
optimization process and as the radiation biology program was expected
to gear-up to try and pin down risk coefficients much better than what
we have right now.
There is still a lot of very large uncertainties in terms of cancer
risk. Frank went to Johnson [NASA] to head up radiation health
protection program and he also serves there as the radiation safety
officer for the astronaut core.
BB:
Last week NASA Director O'Keefe was before a Senate Committee on Space
Science and Transportation describing how deep space radiation can
create health risks for astronauts exposed to radiation sources. Like
Galactic Cosmic Rays (GCR), accelerated proton and electrons to high
energy (E) and high charge (Z) heavy Ions called HZE particles and last
week's Solar Particle Event (SPE). All background radiation throughout
interplanetary space and some trapped inside Van Allan belts. He also
described physiological changes in regards to bone density and muscle
mass loss even through astronauts kept strict health and exercise
regimes in the weightless environment.
How do you see your work as beneficial to protecting astronaut's long
periods of exposure to these health risks in space?
JW: If we are going to have a human exploration program of course this
is a critical issue that has to be solved. O'Keefe recognized when he
first took over the helm of NASA that basically NASA had two high
priority issues that it needed to resolved. One of those is the question
of propulsion providing more efficient propulsion for interplanetary
travel and the other is to provide the necessary protection for the
health of the astronaut against primarily Galactic Cosmic Rays (GCR). It
turns out that Solar Particle Events(SPE) are all that typical to
protect from. The GCR's are very high energy particles that are
streaming into the Solar System and they are very high energy and very
difficult to shield against. And they also consist of particles for
which we have very little information. At one time we had very little
information both from the shielding properties but also from the
biological risk and biological risk are very uncertain for these
particles.
BB: You describe in your paper, "Radiation Shielding Analysis for Deep
Space Missions" as the "Interplanetary Cruise Phase" where Galactic
Cosmic Rays (GCR) and Solar Events Particles (SEP) are encountered.
Could a space vehicle propulsion system providing the best thrust for
speed in-transit to Mars for example reduce astronaut exposure to
"Interplanetary Cruise Phase" GCR and SEP health risks as described in
Cucinotta's operational functional category on risk mitigation? (Since
comparing the "NASA Design Reference Mission" meaning Earth-to-Mars leg
in chemical propulsion would take 6 months as opposed to NTP propulsion
of only 2.5 months or a round trip total of 5 months as compared with 12
months for the NASA plan.)
JW: Once you get on the Mars surface you have two things helping you
out. The first thing is; you are well shielded from GCR's or SPE's
either one because of below the horizon, because of the presence of the
planet itself. So, your main problem of penetration through the
atmosphere which is not very dense on Mars. So you do have a bit of
protection from the atmosphere from the point of view of radiation
protection in space but it's nothing like the Earth's atmosphere which
provides a great deal of protection for us living on the Earth's
surface. On Mars you will see the break-p of a number of the heavy ions
in their penetration through the Mars atmosphere and this is very
helpful within itself. It does generate through a lot of neutrons and it
turns out a lot of those neutrons are produced in the soil underneath
you. The neutrons of course are also very damaging biologically and it
really depends what the ground underneath you is like. If your up in the
polar regions where you have CO2 ice, a lot of CO2 in the ground
underneath you; that is helpful. If you have water ice especially
underground underneath you that's even more helpful. But if your in the
low latitudes planes were it's mainly rock and regolith underneath you
then the neutrons that you see on the surface are mostly produced in the
rock and regolith below the site where your [standing] at.
BB: In transit if you were to take. Let's say...implement a "Direct
Mission Plan" to Mars with a crew of four. The "Powers" that be decided,
they were not going with chemical propulsion. They decide to use a
nuclear thermal propulsion system or even nuclear electrical propulsion
system with on-board neutron sources. Would the tradeoff [to exposure]
be better, using a faster propulsion system so that the exposure
in-transit would be shorter for the astronauts?
JW: Oh, definitely...I was just pointing out that you do have a problem
once you get there to. But it does help a great deal.
BB: You broke down Environment radiation shielding
analysis for manned deep space mission into 4 phases:
-
Interplanetary Cruise Phase
-
Final planetary approach
-
Orbit insertion
-
The surface Phase
In
your estimation from your previous answer; 'The surface phase' would be
detrimental of the four?
JW: It depends on the stay time on the surface and
if it's a relatively short stay then most of your exposure is going to
be in-transit. But, if you have a very long stay on the [Mars] surface
like there have been some scenarios were people may spend as much as a
year in a habitat on surface and then the surface conditions now become
a very important design problem and that is were the neutron problem
come in and play a very important role.
BB: Can you evaluate briefly the MARIE experiment since it was a
platform on the 2001 Mars Odyssey orbiter, in as far as Cruise Phase and
Orbit Phase radiation analysis around Mars ?
JW: The main thing MARIE has been used for is to validate the models
that we use in exposure estimates. Once you place in the corrections for
the structure of the spacecraft itself the agreement between MARIE and
the interplanetary environment and here I'm referring to just the
galactic cosmic ray component have been very very accurate. If you go to
the website: MARIE down at
Johnson Space Center [NASA] often the differences the models and
experiments. We're talking several percent or less.
So, the MARIE instruments has been very helpful providing confidence in
what we're doing. It's mainly been validating the environment models
that we have been using. So far it has been very successful.
BB: So...you've got a good match ?
JW: We have a good match, of course when you have a solar particle event
(SPE) it's different and MARIE has seen a number of SPE events now.
Remember SPE events are almost statistical in nature, it's difficult to
predict ahead of time what an SPE event is going to be like. So, there
are no models there that we can really do any detailed comparisons with.
The best you can hope for is MARIE [data] and the group is working on
this now. Of the solar events that have occurred we have both platforms
are near 1AU of course we have MARIE near Mars and between those two you
can begin to sort out hopefully some of how the particles propagate from
1AU on out to Mars to help you relate all of the observations that we
have seen near Earth and there is a fairly large database on SPE events
near Earth. But how you relate those to what those events would look
like on Mars is still an issue.
BB: You state the Jovian satellite Callisto not
very exciting when compared to Io, Europa, Ganimede but, it is the
safest from a radiation point of view since it's quite distant from the
other moons and Jupiter itself. And that an older male astronaut seem to
fair better career dose limits compared to female astronauts, does
gender make that big of a difference in choosing astronauts for example,
Jovian system human exploration and why?
JW: This has to do with risk coefficients and Frank could discuss more
on this. There's a lot of individual differences in radiation response
of which gender is were we have some of the best studies which really
comes from the Japanese survivors in WWII and there are significant
differences in the cancer induction rate between men and woman. A lot of
this is driven by breast cancer alone which is fairly rare in men. And
it isn't induced by radiation in men as it is in women. There is a
factor of almost two difference. If you look at the paper, "Emerging
Radiation Health Risk Mitigation Technologies" it gives the exposure for
a 3% risk as a function of age for males and females and you'll see that
it gets up to almost a factor of two.
BB: NASA for the last 35 years has collected and monitored the radiation
doses received by all NASA astronauts that traveled into space in fact
some elderly astronauts have returned to space and one Apollo astronaut
had to physically restrain an irate intruder. Proving in some respects
he's in top physical condition. In your estimation have you known an
astronaut that has exhibited out of the ordinary health maladies
attributed to prolonged exposure to space borne radiation?
JW: The problem you have there is the number of astronauts involved is a
very small sample. Even if you look at very large number of workers
say...in the nuclear industry or nuclear weapons development where you
have really large numbers of people involved even then it's difficult.
Of course their exposure levels are much smaller than the astronauts.
The point is, you do need these really large populations to do these
types of studies. Lief Peterson and Frank Cucinotta down at Johnson
Space Center have been doing those type of studies for the astronauts
but the samples are just too small in order to relate to risk, to cancer
risk.
BB: Along those lines what do you think about "Radiation Hormesis" ?
(low doses of irradiation can have a beneficial physiological effect on
the human body for example; chronic exposure exhibited by nuclear
workers had lower cancer mortality rates among general public of the
same profile)
JW: Very controversial...The place where Hormesis has been clearly seen
is in the early radiation response of biological systems. And it does
appear even in single cells but also in whole animals that if you give
them a very low initial exposure of something like x-ray or gamma rays
that you elicit some repair mechanism that start. So, then if you come
in a little while later with a much larger perhaps a lethal exposure.
Then what you find is, they tend to survive better if they got this
early exposure of low dose gamma rays. There is a lot of people that
have seen that type of effect both on a cellular as well as a whole
animal level.
The question is in the case of cancer induction. Which is the primary
risks to astronauts?
The risk coefficients we're using are primarily driven by a cancer risk
and their more driven by mutations and not early death or survival of
the cell. There is the concern even-through the survivability of the
biological system maybe enhanced that you're adding additional mutations
even with these low doses and that is a concern.
BB: I noticed you mention "radiation vaccine" be
close to "radiation hormesis" ?
JW: It's sort of a broader issue and again you find in terms of looking
at the pharmaceuticals. There is dichotomy between the early effects
radiation exposure at very high doses and the effect of long term
exposure. Frank is really the guy to talk more about this. For
pharmaceuticals generally in the past they have been driven mostly by
the military and they're worried about survival on the battlefield and
they're worried about early radiation effects and not so much about
cancer later in life. Where as in astronauts it's about cancer later in
life which is the primary concern.
BB: Excluding the Earth's poles where on Earth are
"hot spots" of natural radiation emission among our continents? Along
those lines, is there tiny specks of decay products of Uranium in space
around Earth ?
JW: There were some high altitude tests both by Russia as well as by the
U.S. In which both fission products as well as uranium and plutonium
went into outer space. Whether there's any still there or not - I don't
know. There is, of course, a small uranium compound in GCR's but it's
very small.
BB: I would think this outer space uranium would have come out of some
kind of volcano or high altitude explosion or supernova maybe stars.
JW: But, those fluxes are very small. In terms of natural radiation on
Earth there are Thorium sands of the coast of India and some places in
Brazil that's "very hot". In Egypt the delta [Nile River Basin].
BB: Does all this bother human beings?
JW: Well, people don't live in those regions most of the time.
Denver is a "Hot Spot" in the U.S. Not as high as the beaches in India.
Even over there in that region their exposure is much higher than most
people around the world and of course they are a real target of doing
studies. Some people who argue Hormesis will point to these areas as no
irradiation effect.
BB: Are you doing some of these studies? (see abstract,
"Overview of Atmospheric Ionizing Radiation (AIR) Research: SST-
Present" available at: www.sciencedirect.com Also
"Overview of Radiation Environments and Human Exposures".)
JW: At the annual meeting of the
NCRP (National Council on Radiation Protection /
ICRP International Commission on
Radiological Protection) in 1998 I was asked to do a summary of human
exposure from the ordinary person, on the terrestrial surface to
Astronauts and what astronauts may be experiencing in the future. That
includes air crew and passengers on airplanes and everything in between.
I tried to cover a fairly broad spectrum.
We have been doing some atmospheric ionizing radiation studies
associated with high speed civil transport. In this report it discusses
some of these issues where the "hot spots" are.
One of the important things from our point of view is. Who is being
exposed by neutrons on the Earth's surface? There's a few places where
the neutron sources are quite a bit higher. That's the capital of
Bolivia.
BB: La Paz.
JW: Same way in Tibet, Lhasa and Denver here in the U.S. Also Leadville
which is the highest village in the U.S.
BB: Uh...Leadville?
JW: Yeah, Leadville, Colorado...It's 11,000 -11,500 feet? They're right
up there. And most of those neutrons are coming from the atmosphere.
BB: You mentioned in your latest paper "Emerging Radiation Health Risk
Mitigation Technologies" that if the body as a magnetic field the dipole
component would make an effective magnetic bottle in which the neutron
charged decay products electrons and protons could be trapped forming a
belt of ionizing radiation centered on the magnetic equator such as for
Earth and Jupiter.
Could a 'mini' electromagnetic Van Allen Belt be artificially
manufactured around a human Mars vehicle in transit thus, funneling most
ionizing radiation on two spots providing crew protection or would the
energy requirements be to expensive to produce?
JW: If you go for a straight dipole and try and use a like super
conducting magnets and so on, you find that's a very difficult problem
to try and protect against GCR rays and the main reason is that they are
so energetic.
The Earth's magnetic field gives us a lot of protection mainly because
it's very extensive. And it isn't that it's a very intense field but,
that it covers a large volume of space that even the small amount of
curvature that it provides to GCR rays does give a lot of protection
inside the magnetic field. You could just see that on the Earth if you
go near the poles substantially higher ionization rates than you do down
at the equator if your on a ship or plane and you see those effects
readily.
The problem is trying to build a large field like that associated with a
spacecraft. There have been some suggestions of using a plasma to
release at the center of the magnetic field to carry it out. Plasma is a
very good conductor and it will grab the "field lines" and tend to pull
them out to very large distances. This has been proposed and the system
is called the "M2P2". So people are suggesting that sort of thing it's
not in the final issue...isn't done yet. But they're both proponents and
those who don't propose that it's going to be helpful.
BB: In Cucinotta's Functional category on radiation health risk
mitigation shielding it states, "At the present time shielding is the
most single counter-measure available." What sort of lightweight
shielding material and their properties qualify and are these
categorizes like: Aluminum, styrofoam, polyethylene, lithium hydride,
liquid hydrogen, hydrogenated graphite nano fibers, water, ice, urine to
name a few and do these scatter radiation enough to render secondary
radiation manageable ?
JW: When we started, his work started in about 1980 and one of the
questions that we wanted to try and resolve at that point was what kind
of material should we be using and of course it largely was in a nuclear
physics issue. So the early part of his work really focused on trying to
define the nuclear physics and defining models that were sufficiently
accurate that you could begin to characterize what shielding materials
were. By 1990 we had a pretty good picture of what was good and what was
not good. Of course the prevailing technology right now is aluminum
alloys. You can apply them well in low Earth orbit and that's mainly
because the protection problem is driven by trapped radiation, once you
get outside the Earth's magnetic field for long periods of time it
appears that aluminum is actually more hazardous. You would think of it
as a shielding material, it actually generates an interior environment
that is even more hazardous than if you didn't have [shielding] anything
there. And that's because of secondary radiation being produced in
collision with the aluminum.
The best material is Liquid Hydrogen .
BB: Gosh...You can use that as fuel ?
JW: Oh yeah...In fact if you look at the study we did for the mission to
Callisto that's basically what we were doing is utilizing hydrogen there
in the fuel tank or in trying to develop a low pressure material and
there's been some preliminary experiments that's been looking promising.
But basically high hydrogen content material, unusually high either from
liquid hydrogen or some sort of nano fiber structure...So that's what we
used there. This is looking forty years out . Now that's the best
material to have.
The question is, if you have to add something with hydrogen what is
best?
Of course Lithium Hydride looks like a very promising material but the
problem is it's not a very good material structurally and so you can
build things out of it. So you try to find things you can build things
with and that brings you into aliphatic polymers (organic compound in
which the carbon atoms are joined in straight chains; as in hexane.) of
which polyethylene is one example were looking at. How can you utilize
polyethylene to build future spacecraft out of and build structures that
are both, damage tolerant to withstand meteorite impact? They have to
have enough strength to withstand the loads from propulsion [production]
and under impact.
Polyethylene has limited structural properties over a fairly limited
range of temperature-this is a problem.
If you look at aromatic polymers these are polymers that have a lot of
ring structures and their fairly good, like polyamides they have a broad
range of temperatures over which they maintain good properties.
So what we're looking into is how we can combine aliphatic and aromatic
into hybrids systems where you can design the temperature and the
strength characteristics to meet your requirements?
So you might think of a craft that's maybe a pure aromatic structure
outside so it has all the good characteristics you need on the outside
to withstand temperature and still support the loads. Then as you come
toward the inside of the craft your changing through various grades of
hybrid structures until you get to the inside and then there would be an
almost pure aliphatic polymer which has good radiation protection
properties as well as structural properties.
BB: What about just plain water or ice?
JW: Well... Water or ice wouldn't withstand loads but water is very
helpful. If we're going to take people you'll have a lot of water on
board so utilizing water tanks is part of the protection system. It is
of course one of the options you want to build into the design process.
One of the options if we went to Mars would be to set-up a methane
production site for the return fuel so you don't have to transport all
that fuel for the vehicle. Methane has very good protection properties
and it's also easy to liquefy much easier than hydrogen.
Lithium Hydride that's a material that normally is integrated into
nuclear reactor shielding designs for space so you're gonna have plenty
of lithium hydride anyway. So you do have that to utilize as well.
The real key is when you build these crafts and your choosing materials.
Chose the materials that meet all your requirements that have the best
radiation protection properties and you have a lot of choices there and
we need to expand those choices so the engineering community when they
do their designs can integrate protection factors into it.
BB: How much of an advantage does the vacuum of
space contribute to the limited reflectability of let's say...On-board
radiation sources of low energy neutron exposure?
JW: When you're using reactor power the streaming especially in space is
very important. Because if you had to build a shield completely
enclosing the reactor the masses get out of hand.
Normally what people do is build a shadow shield and there you have to
minimize the amount of scatter in the shield design that's part of the
design process. Outside that shadow shield the streaming of particles on
out into space is not considered a problem. As long as you don't bring a
human in the vicinity. You have to be very careful in what zone your in.
So you do have a protection problem from that point of view basically,
you work behind a shadow shield.
BB: Do you feel that space radiation mitigation is
a new field and will the need to provide skilled technicians in
verification, testing and safety/risk grow as space mission requirements
become more complex in the future?
JW: Yes, because mostly what NASA has been funding so far is really
small basic research programs to understand what factors are important
in terms of materials. Behind that is a whole engineering process that
requires a lot of technicians, a lot of testing, a lot of development of
how to apply those materials in specific technologies and that problem
is not resolved yet.
That is a big problem, example: polyethylene was identified almost
fourteen, fifteen years ago as probably the best structural type of
material or at least an Aliphatic compound as the best structural
material. But still, there's a huge gap between that identification and
putting it into engineering practice. And it's the engineering practice
that is going to take a fairly long term development and we're going to
need people to work that problem.
BB: Do you think you have some of those people now?
JW: No we don't. We're just in the process of defining things you have
to do, in terms of engineering development. There's really nothing
that's been done yet and there's going to have to be a lot of new
people.
You know...How do you practically fabricate some of these designs
concepts?
It's a real issue.
Because they maybe relatively uniform structures chemically but when you
look at the physical properties they're very in-homogenous. Like, if
you're worried about damage tolerance basically you need a polyethylene
structure that has a hard shell on the outside and a hard shell on the
inside and then it has a lightweight foam in between and the purpose of
that is , the outer shell will fragment meteoroids and once they
fragment they begin to follow cone expansion and as they penetrate past
the first shield you have the fairly lightweight foam to allow them to
expand. So when they hit the inner hard surface the energy is dispersed
over a very large area and it's not likely to penetrate. That's typical
of a wipple shield type structure. But, we have to learn how to build
these things using these new materials, that is not a solved problem
yet.
BB: Could you explain briefly how you got started in this field ?
JW: I became interested in physics when I was a sophomore in college
taking the typical sophomore physics courses.
BB: Which college?
JW: I went to a junior college in my hometown at that point in my junior
year I transferred to Kansas State University in Manhattan, Kansas (the
little apple). That's were I learned computers; computers were pretty
new when I went there. I'm almost sixty three years old, this was back
in the very early sixties and computers were still quite new. I earned a
living, working on a cow project on [Dairies] milk production. And
learned about computers in the process and NASA just happen to come
through interviewing when they found out I had been doing a lot of
research with computers even though on counts they where happy because
few knew what a computer was back then.
Starting with NASA I worked on real time simulation but then became
aware of a fellow named Trutz Foelsche he was a German who came here
after World War II and was interested in the super sonic transport and I
had identified a number of issues with respect to human exposure on
super sonic transport. I started working with him on that problem I then
realized that the transport problem bridges almost all areas of physics
from atomic to nuclear particles so I figured that would be a good
problem to work on.
Soon after that I started to work on a graduate degree from the College
of William and Mary and finally got a Ph.D. degree in heavy ion
interactions and that was the beginning of this work because of the
cosmic ray problem so it just sort of grew out of there.
BB: Thank you, very much...Dr. Wilson for a good interview, it's
refreshing to get NASA technical people to come forward and explain to
the public their work.
JW: The thing I found particularly exciting is the website's student
outreach, I think that's important. Because we need to start worrying
about who's going to fill the ranks of the next generation of technology
people.
BB: I have been told that same thing, a worry that the United States
could fall behind in space technology.
JW: Well...I'm fortunate in my group here [NASA Langley] I have Robert
in his mid forties and another person in his early fifties.
But then I have two young people who are in their early thirties and mid
thirties. So...We have people that are moving up into this area of
expertise now, that are fairly young so we have a pretty good chance of
continuing this effort.
Because I'm not going to continue to work here forever.
BB: Oh...Yeah, I know you need to pass on the [technology] torch,
essentially that's one of the functions of nuclearspace.com is to try
and interest american students to at least train for some of these
endeavors since any up close tangible exhibitions would require someone
to travel to for example; Los Alamos, New Mexico and visit the
Bradbury Science Museum. Because there is no exhibits dedicated to
the use of nuclear power and propulsion in space.
JW: At the "Space 2003 conference" I just got back from there in late
September. That was a very big topic at the conference, basically the
question. Who's going to prepare the next generation of technologies to
carry on space activity? Not only civilian they were also concerned
about military as well as a commercial space activity.
There is a lot of exciting things going on in space science for the
young today I would urge students to look into this as a career.
[
PART II ]
RELATED LINKS:
SPACEWeather.com
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Space Radiation
Shielding |
NASA Space
Radiation Laboratory |
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Space Radiation Analysis
Group NASA |
Spaceflight Radiation Health Program |
| NASA Engineering
Safety Center |
Today's space weather -
NOAA |
HEALTH PHYSICS TERMS LINKS:
NRC
Glossary |
Radiation Related Definitions |
What is
dose? |
Luckey98 Radiation Hormesis |
|
Bobby's Radiation
Glossary |
REFERENCES:
1.John
W.Wilson, Overview of Radiation Environments and Human Exposures, Health
Physics Society vol 79 #5 Nov. 2000, pg.470
2. Kalevi Mursula and Ilya Usoskin, Heliospheric Physics and Cosmic
Rays, pg.1
3.John W.Wilson, Overview of Radiation Environments and Human
Exposures, Health Physics Society vol 79 #5 Nov. 2000, pg.471
4.John W.Wilson, Overview of Radiation Environments and Human
Exposures, Health Physics Society vol 79 #5 Nov. 2000, pg.472
5.John W.Wilson, Overview of Radiation Environments and Human
Exposures, Health Physics Society vol 79 #5 Nov. 2000, pg.473
6.John W.Wilson, Overview of Radiation Environments and Human
Exposures, Health Physics Society vol 79 #5 Nov. 2000, pg.474
7.John W.Wilson, Overview of Radiation Environments and Human
Exposures, Health Physics Society vol 79 #5 Nov. 2000, pg.475
8.John W.Wilson, Overview of Radiation Environments and Human
Exposures, Health Physics Society vol 79 #5 Nov. 2000, pg.476
9.John W.Wilson, Overview of Radiation Environments and Human
Exposures, Health Physics Society vol 79 #5 Nov. 2000, pg.483
10.John W.Wilson, Overview of Radiation Environments and Human
Exposures, Health Physics Society vol 79 #5 Nov. 2000, pg.486
11.John W.Wilson, Overview of Radiation Environments and Human
Exposures, Health Physics Society vol 79 #5 Nov. 2000, pg.490
12.John W.Wilson, J.Miller, A. Konradi and F.A Cucinotta, Shielding
Strategies for Human Space Exploration, NASA CP-3360 publication,
Dec.1997, pg iii, 15-306 (conference publications available at:
NASA STI)
OTHER REFERENCE:
J.W. Wilson, I.W.
Jones, D.L. Maiden, and P. Goldhagen DOE Environmental Measurements
Lab., Atmospheric Ionizing Radiation (AIR): Analysis, Results, and
Lessons Learned From the June 1997 ER-2 Campaign, NASA CP-2003-212155
publication, February 2003 (conference publications available at:
NASA STI)
J.W. Wilson, F.A.
Cucinotta, W. Schimmerling, Emerging Radiation Health-Risk Mitigation
Technologies, [Space Technology and Applications International Forum]
STAIF 2004
J.W. Wilson, W.
Schimmerling, F.A. Cucinotta, J. S. Wood, Effects of Radiobiological
Uncertainty on Vehicle and Habitat Shield Design for Missions to the
Moon and Mars. 1993 NASA technical paper 3312 (available at:
NASA STI)
Myung-Hee Y. Kim,
Sheila A. Thibeault, Lisa C. Simonsen, and J.W. Wilson, Comparison of
Martian Meteorites and Martian Regolith as Shield Material for Galactic
Cosmic Rays, October 1998 NASA TP-1998-208724 (available at:(NASA
STI)
G. De Angelis,
M.S. Clowdsley, J.E. Nealy, R.C. Singleterry, R. T. Tripathi, J.W.
Wilson, Radiation Shielding Analysis for Deep Space Missions, [Space
Technology and Applications International Forum] STAIF 2003 (available
at AIP or local public library)
J.W. Wilson, M.S.
Clowdsley, F.A. Cucinotta, R.K. Tripathi, J.E. Nealy, G. De Angelis,
Deep Space Design Environments for Human Exploration (available at:
LARC search)
J. Wilson photo
courtesy: John Wilson
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