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Surviving in space: the challenges of a manned mission to Mars Lecture 2 Dosimetry and the Effects of the Exposure of Humans to Heavily Ionizing Radiation – PowerPoint PPT presentation

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Title: CERN Course


1
Surviving in space the challenges of a manned
mission to Mars
  • Lecture 2
  • Dosimetry and the Effects of the Exposure of
    Humans to Heavily Ionizing Radiation

2
What Are the Problems Associatedwith Human
Radiation Exposure?
  • Acute (High Intensity-Short DurationDeterministic
    Effects)
  • Serious Debilitation and Death (within Hours to
    Months)
  • NOT GENERALLY THE BIGGEST PROBLEM FACED in Long
    Term Human Space Travel (Because the potential
    sources of this kind of threat are easier to
    mitigate).
  • Chronic (Low Intensity-Long Duration Stochastic
    Effects)
  • Increased Risk of Cancer in the Future
    (Acceptable lt3 Increase)
  • Potential Increased Risk of Other Diseases
    (Coronary, Brain Cell Loss)
  • Increased Risk of Debilitations Like Cataracts
  • THE REAL HURDLE (Due to Bureaucratic Career
    Dose Limits)

3
Contrasting Acute v. Chronic
  • Imagine having to set limits on blood-loss
  • For Acute loss situations over a few hours, the
    amount of loss (without replacement) before
    serious health effects may occur is perhaps as
    much as a few liters
  • On the other hand, for Chronic loss situations
    like blood-donors, one might safely donate one
    liter every 6 weeks, or almost 350 liters over a
    40 year career.
  • The reason for the difference is the human bodys
    ability to replace (blood-loss) and repair
    (radiation damage) in cases of such insults

4
The General Problem
  • NASA needs to be able to PREDICT DOSES or at
    least estimate conservative maximums
  • GCRSolar Modulation Fluctuations
  • (OR any Interstellar Spectral fluctuations???)
  • Solar Particle Events
  • CMEs lower flux events
  • In LEO, Trapped Radiation fluxes are significant
    in low shielding situations

5
A Short Primer on Dose
  • Radiation Dose
  • Energy deposited per gm (cm3) of tissue by
    Ionizing Radiation
  • For Dose D, the Rad (100 ergs/gm) has been
    replaced by
  • the Gray (Gy) J/kg 100 Rad,
  • or more commonly 1 cGy 1 Rad

6
Acute v. Chronic Equivalent Dose
  • Equivalent Dose Dose Modified by Effect in
    Generic Human Tissue
  • Quality Factor Modifiers, WR (RBE) with respect
    to gamma radiations effect for each kind of
    radiation R, summed over all tissues, T HTR
    SR WR DRT
  • For CHRONIC Doses, the Rem has been replaced by
    the Sievert (Sv) 100 Rem
  • For ACUTE Doses, the Dose is given in
    Gray-Equivalent (Gy-Eq) 100 Rads of X-Rays

7
Effective Dose Equivalent
  • Effective Dose Equivalent Uses a Different
    Weighting Factor for EACH kind of tissue, WT ,
    summed over EACH Organ and then over the whole
    body
  • Also quoted in Sieverts (for ChronicStochastic
    Effects)
  • E S WT HT ST WT SR ò WR DRT dT

8
Effects of Dose
  • ACCUTE DOSES (High Short Time Exposures)
  • 4.5 Gy LD 50/60 (50 Lethal in 60 Days)
    without medical intervention
  • 1.0 Gy Radiation Sickness (Nausea, Diarrhea)
  • No Macroscopically Observable effects lt 0.1 Gy
  • CHRONIC DOSES (Low Continual Exposure)
  • Increased Cancer and other risks (Coronary, Eye)
  • No Observable Short-Term effects
  • Long-Term Effects from High LET (Linear Energy
    TransferEnergy deposited per unit track-length
    by ionizing radiation) exposure such as Heavy
    Ions are UNKNOWN
  • Acute Dose Limits are NOT related to Chronic
    Limits

9
Where do we get Data on the Effects of Doses?
  • Actual Human Exposures
  • Hiroshima Survivors represent the best extant
    cohort for long term effects
  • AccidentsSporadic and low statistics.
  • Clinical ExposuresLow Doses or in Radiation
    Therapy exposures, localized high doses No
    Controls
  • Existing Astronaut cohort
  • Animal Exposures
  • Inter-species extrapolation uncertainties
  • Isolated Cell Culture Exposures
  • In Vitro cells do not behave like there
    conterparts In Vivo

10
Energy Loss by Heavy Ions in Tissue
From NASA SPP
11
On The Baseline Mars Mission 1 Fe Traversal PER
CELL
  • The Deep Space GCR Fe 1 per m2 Ster Sec
  • Human Body 1 m2 4p Ster or 10 Fe/sec
  • Baseline Mission 3 Years 108 sec
  • So, there will be 109 Fe traversals per mission
  • 1 m2 1012 mm2 each human cell 103 mm2
  • Or, 109 cells in a typical cross section view
  • Thus, 1 Fe traversal PER CELL !!!
  • The Mission Volunteer Sign-Up Sheet will be
    Available After My Talk

12
DNA-Double Strand BreaksComplex Lesions
Biological Dose
  • The latest idea is that multiple breaks within 30
    base pairs on a DNA strand is a better measure of
    the likelihood of causing a cancer to form than
    other measures of dose.
  • We cannot yet calculate that liklihood from
    first principles.
  • We can estimate it from empirical radiation
    exposure data

13
Current Cancer Risk Model (NCRP-132)
  • 1) Estimates of radiation induced cancer
    mortality are based on the atomic-bomb death
    certificate data for 1950 through 1990.
  • Other human data (reactor workers, patients) used
    as checks for consistency
  • 2) A minimum latency period following exposure
    for radiation induced cancers of 10-years for
    solid cancers is assumed. For leukemia, minimum
    latency of 2-years, however risks are multiplied
    by 0.1, 0.25, 0.5, 0.75, 0.9, and 1 for years 3,
    4, 5, 7, and 8 or more years after exposure,
    respectively.
  • 3) The excess relative risk for solid cancer is
    assumed to be constant over time following
    exposure. For leukemia a decline in excess risk
    with time after exposure is assumed.
  • 4) The baseline survival and cancer rates for
    astronauts are assumed as those of the US
    population (SEER, 2000).

Slide Courtesy of F. Cucinotta, NASA/JSC
14
Current Cancer Risk Model (NCRP-132)(Continued)
  • 5) The transfer of risk from the Japanese to the
    US population for solid cancers is made using the
    average of the multiplicative and additive
    transfer models, and for leukemias using the
    additive transfer model.
  • 6) The dose response for the acute exposures of
    the Japanese survivors is assumed to be a linear
    function of dose. For leukemia a linear-quadratic
    dose response function is used.
  • 7) For chronic exposures a dose and dose-rate
    reduction factors of two is assumed. The
    quadratic term in the leukemia response model is
    set to zero.
  • 8) For high-LET radiation, an LET dependent
    radiation quality factor, Q(L) recommended by the
    ICRP is used to scale the doses (No other factors
    in the model are assumed to depend on radiation
    quality).

Slide Courtesy of F. Cucinotta, NASA/JSC
15
Current Model- continued
  • q(a) probability to die for age a and a1 based
    on US mortality rate, M (all causes) and exposure
    dependent cancer rate, m
  • Probability to survive to age a
  • Mortality rate for ion fluence F, of LET, L
    (ntransfer model weight)
  • Excess Lifetime Risk (ELR)
  • Risk of Exposure Induced-Death (REID)

Slide Courtesy of F. Cucinotta, NASA/JSC
16
Transfer ModelsAvailable data? Populations ?
Individuals
  • Cohort baseline BJ (unexposed group)
  • US Baseline BA
  • aA linear coefficient fit to exposed cohort
  • Additive Transfer
  • RiskA BA aJ x Dose
  • Multiplicative Transfer
  • RiskM BA/ BJ x aJ x Dose
  • Accuracy?
  • large variations for specific tissue sites
  • healthy workers or individuals
  • genetic background
  • dietary/environmental
  • untested for space radiation non-cancer risks

Additive Transfer radiation acts independent
of spontaneous cancer risks Multiplicative
Transfer radiation risk depends on spontaneous
cancer risks
LSS Transfer to US (NCRP Report 126)
Slide Courtesy of F. Cucinotta, NASA/JSC
17
Methods for Uncertainty Estimates
  • Method Monte Carlo sampling over each factor in
    model based on current knowledge to form
    Probability Distribution Function (PDF)
  • PDF defined to bound values of each factor
    (quantile) x
  • Cancer mortality rate for ions
  • Physics PDF based on comparisons to flight data
  • Use of REID corrects for competing risks
    (important for Mars mission)

Factors (NCRP 126) xD DS86 (dosimetry of
A-bombs) xS Statistical errors xT pop.
transfer xP Bias xDr Dose-rate effects xQ
Quality factors xL physics (transport/dosimetry)

Slide Courtesy of F. Cucinotta, NASA/JSC
18
Radiation Quality Effects
  • Tradition- Effects increase to about 100-200
    keV/mm and then decline due to overkill
  • Mechanisms
  • Energy deposition in Biomolecules
  • Cluster DNA damage site
  • Gene deletion/mutation
  • Chromosomal aberrations
  • Sterilization term in dose-response
  • Genomic instability
  • LET or dose thresholds in activating molecular
    pathways (epigenetic effects)

Cell Death is good
Slide Courtesy of F. Cucinotta, NASA/JSC
19
Uncertainties in Biological Effectiveness
  • Trial Function, Q(L)
  • Sampling
  • L0 1, 15 (flat 5 to 10)
  • Lm 50, 250 (flat 80 to 150)
  • Declining slope, p 0,2
  • Qp 30 log-normal with GSD1.8
  • Space missions-trial Q convoluted with trial LET
    spectra to form sample rate

Slide Courtesy of F. Cucinotta, NASA/JSC
20
Accuracy of Physics Models 20(environments,
transport, shielding)
ISS Mission
Slide Courtesy of F. Cucinotta, NASA/JSC
21
PDF for Physics Uncertainties- GCR
Slide Courtesy of F. Cucinotta, NASA/JSC
22
Fatal Cancer Risk per Rad vs. LET
  • Average Life-loss from radiation cancer death
  • (40-yr at exposure) low LET
  • Leukemia 20 yr
  • Solid Cancers
  • Multiplicative Transfer 12-yr
  • Additive Transfer 20-yr
  • HIGH LET???

Slide Courtesy of F. Cucinotta, NASA/JSC
23
Uncertainties not Included
  • Deviation from linear-additivity models
  • Radiation quality and latency or progression
  • Models assume a constant ERR (Equivalent Relative
    Risk) for solid cancers with no time-dependence
    on radiation quality
  • Animal and cellular models suggest decreased
    latency with increasing LET and ERR declines
    after saturation
  • Possible uncertainties for mixed fields and
    progression not modeled
  • Radiation quality and susceptibility
  • Population averaged values do not account for
    dispersion due to genetic factors (familial, high
    and low penetrance genes, SNPs-Single Nucleotide
    Polymorphisms)
  • Neutron carcinogenesis studies show RBE
    variations across mouse strains for same tissue
  • Non-cancer mortality
  • Dose limits need to consider life-loss per death
    across each cause
  • For Mars mission non-cancer risks may be a
    significant competing risk to radiation
    carcinogenesis

Slide Courtesy of F. Cucinotta, NASA/JSC
24
High LET- Protraction Effects
Pulmonary Tumors - fission neutrons in B6CF1
mice (Fry et al., Env. Int. 1, (1972))
Slide Courtesy of F. Cucinotta, NASA/JSC
25
Radiation Risqué- transgender estimates(M(a)
Net Mortality MC(a) Cancer Mortality)
Differences between males and females are
approximate level of change for calendar year
changes
Slide Courtesy of F. Cucinotta, NASA/JSC
26
Summary of Issues
  • Acute effects are more predictable than Chronic
    effects for Space Radiation Exposures
  • Cancer Risk is the Primary Chronic Effect.
  • Big uncertainties exist in estimating risks
    because
  • Effects from high LET radiation are poorly known
  • Cancer causes themselves are not well understood.
  • Current Policies Require Limiting Risks to the
    same values as for Earth-based workers.

27
Possible Strategies
  • Classical Solutions Time, Shielding Distance
  • Distancewe can do nothing about
  • TimeMore powerful rockets to reduce mission
    durations and thus exposure time
  • ShieldingDoable from the physics standpoint but
    Expensive from the standpoint of weight ( )
  • Long Surface StaysUse local soil overburden as
    shielding material
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