fundamentals of decompressionspacecraft.ssl.umd.edu/academics/697s11/697s11l07... · fundamentals...
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Fundamentals of Decompression• History• Tissue models
– Haldane– Workman– Bühlmann
• Physics of bubbles• Spacecraft cabin atmospheres
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© 2011 David L. Akin - All rights reservedhttp://spacecraft.ssl.umd.edu
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
First Class Assignment• Four topics in the first section of the course
– Space Habitability– Human Factors – Anthropometrics– Psychosocial Aspects
• Find a technical paper in two of the topic areas• Post the paper (in PDF) and a summary (~0.5-1
page) to discussion board on Blackboard• No duplication! There’s an advantage in being first• Due Thursday March 3rd
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Discussion of Term Project• Please go to Blackboard site and list team members
(and innovative team names) for all teams• First phase: design interior layout of X-Hab in
configuration for 2011 test series– Accommodations for four crew– Diagrams coming for outer envelope
• Submit as slide package (no presentation) by March 18 (i.e., before Spring break)
• Second phase: full interior layout of two layers with life support and habitat elements
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Caissons• Pressurized chambers
for digging tunnels and bridge foundations
• Late 1800’s - caisson workers exhibited severe symptoms– joint pain– arched back– blindness– death
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Brooklyn Bridge• Designed by John Roebling, who
died from tetanus contracted while surveying it
• Continued by son Washington Roebling, who came down with Caisson Disease in 1872
• Competed by wife Emily Warren Roebling
• 110 instances of caisson disease from 600 workers
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Decompression Sickness (DCS)• 1872 - Dr. Alphonse Jaminet noted similarity
between caisson disease and air embolisms• Suggested procedural modifications
– Slow compression and decompression– Limiting work to 4 hours, no more than 4 atm– Restricting to young, healthy workers
• 1908 - J.B.S. Haldane linked to dissolved gases in blood and published first decompression tables
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Supersaturation of Blood Gases• Early observation that “factor of two” (50% drop in
pressure) tended to be safe• Definition of tissue ratio R as ratio between
saturated pressure of gas compared to ambient pressure
• 50% drop in pressure corresponds to R=1.58(R values of ~1.6 considered to be “safe”)
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R =PN2
Pambient= 0.79 (nominal Earth value)
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Tissue Models of Dissolved Gases• Issue is dissolved inert gases (not involved in
metabolic processes, like N2 or He)• Diffusion rate is driven by the gradient of the
partial pressure for the dissolved gas
where k=time constant for specific tissue (min-1)P refers to partial pressure of dissolved gas
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dPtissue(t)dt
= k [Palveoli(t)− Ptissue(t)]
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Solution of Dissolved Gas Diff. Eq.• Assume ambient pressure is piecewise constant
(response to step input of ambient pressure)• Result is the Haldane equation:
• Need to consider value of Palveoli
where Q=fraction of dissolved gas in atmosphere ΔPO2=change in ppO2 due to metabolism
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Ptissue(t) = Ptissue(0) + [Palveoli(0)− Ptissue(0)]�1− e−kt
�
Palveoli =�
Pambient − PH2O +1−RQ
RQPCO2
�Q
Palveoli = (Pambient − PH2O − PCO2 + ∆PO2)Q
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Linearly Varying Pressure Solution• Assume R is the (constant) rate of change of
pressure - solution of dissolved gases PDE is
• This is known as the Schreiner equation • For R=0 this simplifies to Haldane equation• Produces better time-varying solutions than
Haldane equation• Easily implements in computer models
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Pt(t) = Palv0 + R
�t− 1
k
�−
�Palv0 − Pt0 −
R
k
�e−kt
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Tissue Saturation following Descent
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Tissue Saturation after Ascent
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Effect of Multiple Tissue Times
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Haldane Tissue Models• Rate coefficient frequently given as time to evolve
half of dissolved gases:
• Example: for 5-min tissue, k=0.1386 min-1• Haldane suggested five tissue “compartments”: 5,
10, 20, 40, and 75 minutes• Basis of U. S. Navy tables used through 1960’s• Three tissue model (5 and 10 min dropped) • 1950’s: Six tissue model (5, 10, 20, 40, 75, 120)
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T1/2 =ln (2)
kk =
ln (2)T1/2
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Workman Tissue Models• Dr./Capt. Robert D. Workman of Navy
Experimental Diving Unit in 1960’s• Added 160, 200, 240 min tissue groups• Recognized that each type of tissue has a differing
amount of overpressure it can tolerate, and this changes with depth
• Defined the overpressure limits as “M values”
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Workman M Values• Discovered linear relationship between partial
pressure where DCS occurs and depth
M=partial pressure limit (for each tissue compartment)M0=tissue limit at sea level (zero depth)ΔM=change of limit with depth (constant)d=depth of dive
• Can use to calculate decompression stop depth
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M = M0 + ∆Md
dmin =Pt −M0
∆M
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
PADUA (Univ of Penn.) Tissue ModelTissue T1/2 (minutes) M0 (bar)
1 5 3.0402 10 2.5543 20 2.0674 40 1.6115 80 1.5816 120 1.5507 160 1.5208 240 1.4909 320 1.490
10 480 1.459
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Bühlmann Tissue Models• Laboratory of Hyperbaric Physiology at University
Hospital, Zurich, Switzerland• Developed techniques for mixed-gas diving,
including switching gas mixtures during decompression
• Showed role of ambient pressure on decompression (diving at altitude)
• Independently developed M-values, based on absolute pressure rather than SL depth
• “Zurich” 12 and 16-tissue models widely used
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Bühlmann M-Value Models• Modifies Workman model by not assuming sea
level pressure at water’s surface
Pamb=pressure of breathing gasb=ratio of change in ambient pressure to change in tissue pressure limit (dimensionless)a=limiting tissue limit at zero absolute pressure
• ZH-L16 model values for a and b
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M =Pamb
b+ a
a = 2 T− 1
31/2 < bar > b = 1.005− T
− 12
1/2
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Physics of Bubbles• Pressure inside a bubble is balanced by exterior
pressure and surface tension
where γ=surface tension in J/m2 or N/m (=0.073 for water at 273°K)
• Dissolve gas partial pressure Pg=Pamb in equilibrium
• Gas pressure in bubble Pint>Pamb due to γ• All bubbles will eventually diffuse and collapse
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Pinternal = Pambient + Psurface = Pambient +2γ
r
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Critical Bubble Size• Minimum bubble size is defined by point at which
interior pressure Pint = gas pressure Pg
• r<rmin - interior gas diffuses into solution and bubble collapses
• r>rmin - bubble will grow • r=rmin - unstable equilibrium
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rmin =2γ
Pg − pambient
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Bubble Formation and Growth• In equilibrium, external pressure balanced by internal
gas pressure and surface tension• Surface tension forces inversely proportional to radius
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
“Clinical” Discussion of DCS• Tissue models are predictive, not definitive• Every individual is different
– Overweight people more susceptible to DCS– Tables and models are predictive limits - there will be
“outliers” who develop DCS while adhering to tables
• Doppler velocimetry reveals prevalence of bubbles in bloodstream without presence of DCS symptoms - “asymptomatic DCS”
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Implications of DCS in Space Flight• Drop from sea level pressure to ~4 psi, 100% O2
pressure– Equivalent to ascent from fully saturated 120 ft dive – Launch in early space flight– Extravehicular activity from shuttle or ISS
• To have “safe” (R=1.4) EVA from shuttle requires suit pressure of 8.2 psi
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R =PN2
Pamb=
14.7(0.78)4
= 2.87
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Current Denitrogenation Approaches• Depress to 10.2 psi for 12-24 hours prior to EVA
– Full cabin depress in shuttle– “Campout” in air lock module of ISS
• Exercise while breathing 100% O2• In-suit decompression on 100% O2 (3.5-4 hours)
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Historical Data on Cabin Atmospheres
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from Scheuring et. al., “Risk Assessment of Physiological Effects of Atmospheric Composition and Pressure in Constellation Vehicles” 1 6th Annual Humans in Space, Beijing, China, May 2007
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Spacecraft Atmosphere Design Space
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from Scheuring et. al., “Risk Assessment of Physiological Effects of Atmospheric Composition and Pressure in Constellation Vehicles” 1 6th Annual Humans in Space, Beijing, China, May 2007
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Effect of Pressure and %O2 on Flammability
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from Hirsch, Williams, and Beeson, “Pressure Effects on Oxygen Concentration Flammability Thresholds of Materials for Aerospace Applications” J. Testing and Evaluation, Oct. 2006
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
U N I V E R S I T Y O FMARYLAND
Atmosphere Design Space with Constraints
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from Scheuring et. al., “Risk Assessment of Physiological Effects of Atmospheric Composition and Pressure in Constellation Vehicles” 1 6th Annual Humans in Space, Beijing, China, May 2007
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Fundamentals of DecompressionENAE 697 - Space Human Factors and Life Support
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Constellation Spacecraft Atmospheres
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from Scheuring et. al., “Risk Assessment of Physiological Effects of Atmospheric Composition and Pressure in Constellation Vehicles” 1 6th Annual Humans in Space, Beijing, China, May 2007