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Possible Temperature-RelatedPossible Temperature-Related
SlopeSlope
and Surface Roughnessand Surface Roughness
DifferencesDifferences
Between the North and South WallsBetween the North and South Walls
of Coprates Chasma, Marsof Coprates Chasma, Mars
joern@jernsletten.namejoern@jernsletten.name
http://joern.jernsletten.name/http://joern.jernsletten.name/
Tirsdag, 15. Juni 2004Tirsdag, 15. Juni 2004
Universitetet i BergenUniversitetet i Bergen
Det Matematisk-Naturvitenskapelige FakultetDet Matematisk-Naturvitenskapelige Fakultet
Institutt for GeovitenskapInstitutt for Geovitenskap
DoctorDoctor
PhilosophiaePhilosophiae
DisputaDisputa
ss
JJøørn Atlern Atle
JernslettenJernsletten
OutlineOutline
• Questions?
• Geology and stratigraphy of Valles Marineris /
Coprates Chasma
• Creep of ice-rich geologic materials
– Deformation mechanisms
– Temperature dependence in material strength
– Earth / Mars analogs
• MOLA data
• Topographic architecture of Coprates Chasma
• Topographic profiling methods
• Data and statistics
• Conclusions
Questions?Questions?
• Effect of temperature on topography of the
near-equatorial trough of Coprates Chasma?
• Presence of ground ice and its role in
landscape evolution?
• Over geologic time, surface temperature factor in:
– Rheology and stability of ice-rich geologic materials
– Evolution and morphology of the trough walls
– Controlling the distribution of ground ice
• Do expected temperature differences result in:
– Measurable differences in slope angles?
– Measurable differences in surface roughness?
Chronology Based on Crater CountsChronology Based on Crater Counts
( Adapted from McKee, 2003, after: Hartman and Neukum, 2001;
Jakosky and Phillips, 2001; Zuber, 2001; Tanaka et al., 1992 )
Global Map of MarsGlobal Map of Mars
( Modified from Eötvös Lor( Modified from Eötvös Loránd University, 2001 )nd University, 2001 )
Geologic Map LegendGeologic Map Legend
√
√
√
√
( Created from GIS tabular data from Scott and Tanaka, 1986 )( Created from GIS tabular data from Scott and Tanaka, 1986 )
√
√
Valles Marineris Geologic MapValles Marineris Geologic Map
( Modified from Scott and Tanaka, 1986 )
Coprates Chasma Layering andCoprates Chasma Layering and
Spur-and-Gully MorphologySpur-and-Gully Morphology
b. This close-up is centered at 14.5° South, 55.8° West;
Image covers an area of approximately 9.8 km by 17.3
km;
North is up ( MOC images courtesy of NASA/JPL/Malin
Space Science Systems )
a. Context image b. Central ridge close-up
StressStress // Strain RelationshipsStrain Relationships
μ = ε1
/ε3 Equation 4.3
Poisson’s ratio, μ, ratio of unit strain perpendicular and parallel
to applied stress:
Poisson’s ratio describes the ability of a solid to shorten parallel to σ1
without
elongation in the σ3
direction, and can vary from 0 (compressible) to 0.5
(incompressible)
In the case of ideally viscous (Newtonian) materials, strain rate
is related in a linear fashion to applied stress:
σ = ηέ Equation 4.4
where η is the viscosity, a material property constant
During steady state creep, the stress and strain rate are related in
a power law:
έ = A exp –(Q/RT)σN Equation 4.5
where T is the absolute temperature; A is a temperature-dependent constant, the
frequency factor; Q is a constant, the activation
energy for creep; R is the universal gas constant; and N is the
stress exponent, typically varying from 1-2 when σ is < 20 MPa, and
from 2-4 when 20 < σ < 200 MPa
Map of the Deformation Mechanisms of IceMap of the Deformation Mechanisms of Ice
As a function of temperature, applied stress, and strain rate
( from Carr, 1996, after Shoji and Higashi, 1978 )
Constitutive Relation for IceConstitutive Relation for Ice
Glen's Flow Law is widely accepted as the constitutive relation
for ice when shear stress acts on its basal plane:
where έ is the strain rate; A is a temperature-dependent constant; τb
is the basal shear stress; and n is a power law exponent (Glen, 1958)
έ = A τb
n
Equation 4.15
 Regards ice as a plastic substance with a yield stress τ of 1 bar
(Paterson, 1981)
 Value of n generally taken as 3 (Paterson 1981; Johnston, 1981)
 Shear strain rate (flow velocity) is lower for colder ice as a
function of A
 A varies with temperature, and is equal, for example, to 6.8 x 10 -15
s-1
kPa-3
at 273 K, 4.9 x 10-16
at 263 K, 1.7 x 10-16
at 253 K, and 5.1
x 10-17
at 243 K
 n varies with applied stress, taking a value of 1 for Newtonian
deformation, and 3 for non-Newtonian deformation (Paterson, 1994)
 Available evidence indicates that n = 3 for most situations
(Russell-Head and Budd, 1979)
Deformation of Frozen GroundDeformation of Frozen Ground
The total strain in deforming frozen ground is the sum of an
instantaneous strain, ε(i)
, and a creep strain, ε(c)
. The primary
creep of frozen ground (and ice) in a state of constant stress
can be described by the creep law (Andersland et al., 1978):
ε(c)
= Kσn
tb
Equation 4.17
where K, n, and b are temperature-dependent material constants
The steady state creep strain is governed by the creep law
(Hult, 1966):
έ(c)
= G(σ, T) Equation 4.18
where έ(c)
is the steady state (secondary) creep rate; and the
function G(σ,T) is found by plotting the slope dε(c)
/dt against
the applied stress for various temperatures
Temperature Dependence inTemperature Dependence in
the Creep Lawthe Creep Law
where έc
is the creep rate selected for the laboratory experiment
- for frozen soils is often taken as 10-5
min-1
(Andersland et al.,
1978); σc
is the uniaxial stress for the selected creep rate; σc
(T) and n(T) are
temperature-dependent creep parameters
The creep law can be rewritten in the form of a power expression
(Hult, 1966; Ladanyi, 1972):
έ(c)
= έc
[σ/σc
(T)]n(T)
Equation 4.19
 The equations for both primary and secondary creep emphasize the
temperature-dependence of creep deformation
Dependence on Temperature ofDependence on Temperature of
CompressiveCompressive
Strength for Ice and Various Frozen SoilsStrength for Ice and Various Frozen Soils
( From Andersland et al., 1978;
after Sayles, 1966 )
Debris-Ice Feature TerminologyDebris-Ice Feature Terminology
( Adapted from Whalley and Azizi, 2003 )
Typical Rock Glaciers inTypical Rock Glaciers in
Wrangell Mountains, AlaskaWrangell Mountains, Alaska
Rock glacier “a” has a single lobe, and rock glacier “b”
has a second lobe that appears to have advanced on
top of another lobe that advanced at an earlier time
( Adapted from Whalley and Azizi, 2003 )
Two Possible Rock-Ice SystemsTwo Possible Rock-Ice Systems
in Candor Chasma, Marsin Candor Chasma, Mars
Feature “A” resembles a rock glacier, and feature
“B” resembles a protalus rampart
( Adapted from Whalley and Azizi, 2003;
After Malin et al., 2000 )
Enlargements of Candor ChasmaEnlargements of Candor Chasma
FeaturesFeatures
Feature “A” resembles a rock glacier, and feature
“B” resembles a protalus rampart
( Adapted from Whalley and Azizi, 2003;
After Malin et al., 2000 )
Enlargement of feature A Enlargement of feature B
Mars Orbiter Laser AltimeterMars Orbiter Laser Altimeter
(MOLA) Data(MOLA) Data
• Polar orbit
• Nadir measurements
• ±30 cm vertical accuracy
• ~150 m spot size
• ~330 m along-track spacing
(along orbital track)
• Good coverage in Valles Marineris region
1/641/64°° Gridded MOLA ElevationGridded MOLA Elevation
DataData
• 1/64° resolution ≈ 926 m/pixel
• Elevation: ±30 cm vertical accuracy
• Steepest gradient slope angle
• Steepest gradient slope aspect
(slope orientation)
• Measures of surface roughness:
– Curvature (slope of slope)
– Surface area ratio (ratio of total surface area
to planimetric surface area)
• Intermediate products:
– Cosine (aspect)
– North-South component of slope angle
– Local incidence angles
• Temperatures
247 Profiles Across Coprates247 Profiles Across Coprates
ChasmaChasma
Coprates Chasma Trough Wall Cutout marked on this map is the location of the trough wall segment in
Figure 6.2. The points marked in green are the starting points for each profile, while the points in red are
correspondingly the end points for each profile. From west to east, the two profiles marked in bright red
are Coprates Chasma profile number 100 and Coprates Chasma profile number 200, respectively
Basic Topographic Architecture ofBasic Topographic Architecture of
Coprates ChasmaCoprates Chasma
• Extends from 54º to 70º West longitude
• 10º to 17º South latitude
• ~1,000 km long
• Trough trends 100º-104º
• Elevations at trough rims range from 0.5 km below
datum to 5.5 km above datum
– Highest elevations along the segment of the trough
extending from 64º to 67º West longitude
• Width of trough ranges from 70 km to 125 km
• Trough wall heights vary from ~4.5 km to ~10.5 km
– Deepest segment of the trough extending from 64º to 67º
West longitude
Structural Cross-Section ofStructural Cross-Section of
Coprates ChasmaCoprates Chasma
( Adapted from Schultz, 1991 )
Steepest Gradient Slope Angles andSteepest Gradient Slope Angles and
AspectsAspects
 Arrow on trough wall points in direction of steepest gradient
 Slope angle is calculated in this direction
 Slope aspect is the horizontal direction (bearing) in which the arrow
points
Topographic Profiling RulesTopographic Profiling Rules
1) The trough rim, coming in either direction (~north or
~south) is the first point steeper than 5° where it and the
next 14 points (15 points total) average > 8.75°
2) Points selected for analysis must:
a) Be located between the rim and the first point at which elevation is <= rim
elevation minus 50% of the difference between the rim elevation at that
side of the trough (north or south) and the absolute lowest elevation
anywhere along the profile (inclusive)
b) Have slope aspects within +/- 60° (non-inclusive) of profile trend (for most
Coprates profiles, ~194° trend coming from north, correspondingly ~14°
trend coming from south)
c) Have slope angles > 5°
3) Each of the 5 topographic parameters (elevation, slope
angle, slope aspect, curvature, surface area ratio) is
averaged in a "selective average" over the wall segment
extracted according to 2) as follows:
a) The sum of values of the parameter at all points satisfying 2) rules
b) The count of points satisfying 2) rules
c) a) divided by b) for north and south trough walls, respectively
4) Going downslope, find the first 5 points averaging < 3.7º,
last of the 5 is the trough wall bottom
Valid Points for Analysis AlongValid Points for Analysis Along
Coprates Chasma Profile NumberCoprates Chasma Profile Number
200200
 Vertical exaggeration = 6x
 Profile aspect = 187.2º (North wall) / 7.2º (South wall)
Cryosphere and Thermal EquationsCryosphere and Thermal Equations
g
msmp
Q
ΤΤ
z
−
Κ=
 
Equation 3.1
 
Tms
= 64 K cos i + 154 K Equation 6.2
where z is depth, K is the thermal conductivity of the Martian crust, Tmp
is the
melting point of ground ice, Tms
is the (latitude-dependent) mean annual surface
temperature, and Qg
is the value of the geothermal heat flux. Nominal values
cited for Mars are Qg
= 30 mW m-2
, K = 2.0 W m-1
K-1
, and Tmp
= 252 K (Clifford,
1993)
Steady state one-dimensional heat conduction equation:
Simplified surface energy balance equation (Equation 6.1):
where i is the local incidence angle; assuming an albedo of Ab = 0.25, a thermal
conductivity of k = 2.0 W m-1
K-1
, and ignoring the latent heat of CO2 sublimation
(L); works well equatorward of approximately 45º north or south latitude
Thermal EquationsThermal Equations
4
2
0
cos)1( T
dt
dm
LF
z
T
kiA
R
S
ab εσ=++
∂
∂
+− Equation 6.1
i = abs (l - β) Equation 6.3
β = s cos a Equation 6.4
Surface energy balance equation:
where S0
is the solar constant at 1 AU, R is the mean distance of Mars from the
sun, Ab
is the bolometric albedo, i is the local incidence angle of sunlight, k is the
thermal conductivity of the regolith, Fa
is the downward component of atmospheric radiation, L is the latent
heat of CO2
sublimation, m is the mass of CO2
condensate per unit area, ε is the
surface emissivity, σ is the Stephan-Boltzmann constant, and
T is temperature (Kieffer et al., 1977; Clifford, 1993)
Local incidence angle:
where i is the local incidence angle, l is latitude, and β is the
north-south component of slope
North-south component of slope:
where β is the north-south component of slope s is slope angle, and a
is slope aspect (slope orientation)
Temperature vs. Incidence AngleTemperature vs. Incidence Angle
Coprates Chasma TemperatureCoprates Chasma Temperature
DataData
Temperature vs. LongitudeTemperature vs. Longitude
Temperature was calculated using Equation 6.2, Equation 6.3,
and Equation 6.4
Temperature Along CopratesTemperature Along Coprates
Chasma Profile Number 200Chasma Profile Number 200
 Vertical exaggeration of elevation profile = 5x
Calculated Possible Depths to theCalculated Possible Depths to the
Base of the Martian CryosphereBase of the Martian Cryosphere
( Adapted from tabular data, Clifford, 1993 ). The thermal model
used Equation 3.1, and with the following values for parameters:
Minimum: Qg
= 45 mW m-2
, K = 1.0 W m-1
K-1
, and Tmp
= 210 K;
Nominal: Qg
= 30 mW m-2
, K = 2.0 W m-1
K-1
, and Tmp
= 252 K;
Maximum: Qg
= 15 mW m-2
, K = 3.0 W m-1
K-1
, and Tmp
= 273 K
Coprates Chasma Profile Number 200Coprates Chasma Profile Number 200
with Hypothetical Cryospherewith Hypothetical Cryosphere
Calculated using Equation
3.1;
Nominal values cited for Mars
are Qg
= 30 mW m-2
, K = 2.0
W m-1
K-1
, and Tmp
= 252 K
(Clifford, 1993);
Tms
was calculated using
Equation 6.2, Equation 6.3,
and Equation 6.4
a. 6x vertical exaggeration
b. No vertical exaggeration
3.6 km 2.2 km
Coprates Chasma Slope Angle vs.Coprates Chasma Slope Angle vs.
Longitude for North and South WallsLongitude for North and South Walls
Coprates Chasma Slope AngleCoprates Chasma Slope Angle
DifferencesDifferences
Coprates Chasma Curvature vs.Coprates Chasma Curvature vs.
LongitudeLongitude
Coprates Chasma Surface Area RatioCoprates Chasma Surface Area Ratio
vs. Longitudevs. Longitude
Paired Differences Between NorthPaired Differences Between North
and South Wall Dataand South Wall Data
Elevations of Coprates ChasmaElevations of Coprates Chasma
Floor and Surrounding PlateausFloor and Surrounding Plateaus
Coprates Chasma Trough RimCoprates Chasma Trough Rim
Elevation vs. LongitudeElevation vs. Longitude
Coprates Chasma Trough WallCoprates Chasma Trough Wall
Height vs. LongitudeHeight vs. Longitude
Coprates Chasma Trough Wall BottomCoprates Chasma Trough Wall Bottom
Elevations for North and South WallsElevations for North and South Walls
Coprates Chasma Trough Wall BottomCoprates Chasma Trough Wall Bottom
ElevationsElevations
• There is NO significant difference
in elevation between the North and
South trough wall bottoms
• The place is FLAT!
Slope Angle Correlations WithSlope Angle Correlations With
Morphological and Structural PatternsMorphological and Structural Patterns
Morphologic and structural
patterns are from Peulvast et
al. (2001)
Morphology Key
(1) Cornice with smooth talus
slope;
(2) Cornice with spurs and
gullies;
(3a) Crest with spurs and
gullies on both sides;
(3b) Crest with spurs and
gullies on one side and
smooth talus slope on
the other side;
Structure Key
(4a) Fault;
(4b) Conjectured fault;
(5a) Normal fault;
(5b) Conjectured normal fault
Coprates Chasma Trough Wall HeightCoprates Chasma Trough Wall Height
vs. Slope Anglevs. Slope Angle
( Results of Schultz, 2002 Superimposed on Results from this Study;
Mége and Gatineau, 2003: RMR = 50-70 )
ConclusionsConclusions
• North walls of Coprates Chasma 1.33º ± 0.49º
steeper than South walls
• No significant difference in curvature between
North walls and South walls
• Surface area ratios 0.011 ± 0.004 higher in the
North walls than in the South walls
• Cryosphere thickness
– ~3.7 km in North walls
– ~2.3 km in South walls
• ~10 K temperature difference
• Similarities between walls
– Horizontal stratigraphic layers
– Spur-and-gully morphology
– Apparently similar materials
– Geology
• Extremely flat trough floor
• Tectonic symmetry

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Dr.Philos._Disputas

  • 1. Possible Temperature-RelatedPossible Temperature-Related SlopeSlope and Surface Roughnessand Surface Roughness DifferencesDifferences Between the North and South WallsBetween the North and South Walls of Coprates Chasma, Marsof Coprates Chasma, Mars joern@jernsletten.namejoern@jernsletten.name http://joern.jernsletten.name/http://joern.jernsletten.name/ Tirsdag, 15. Juni 2004Tirsdag, 15. Juni 2004 Universitetet i BergenUniversitetet i Bergen Det Matematisk-Naturvitenskapelige FakultetDet Matematisk-Naturvitenskapelige Fakultet Institutt for GeovitenskapInstitutt for Geovitenskap DoctorDoctor PhilosophiaePhilosophiae DisputaDisputa ss JJøørn Atlern Atle JernslettenJernsletten
  • 2. OutlineOutline • Questions? • Geology and stratigraphy of Valles Marineris / Coprates Chasma • Creep of ice-rich geologic materials – Deformation mechanisms – Temperature dependence in material strength – Earth / Mars analogs • MOLA data • Topographic architecture of Coprates Chasma • Topographic profiling methods • Data and statistics • Conclusions
  • 3. Questions?Questions? • Effect of temperature on topography of the near-equatorial trough of Coprates Chasma? • Presence of ground ice and its role in landscape evolution? • Over geologic time, surface temperature factor in: – Rheology and stability of ice-rich geologic materials – Evolution and morphology of the trough walls – Controlling the distribution of ground ice • Do expected temperature differences result in: – Measurable differences in slope angles? – Measurable differences in surface roughness?
  • 4. Chronology Based on Crater CountsChronology Based on Crater Counts ( Adapted from McKee, 2003, after: Hartman and Neukum, 2001; Jakosky and Phillips, 2001; Zuber, 2001; Tanaka et al., 1992 )
  • 5. Global Map of MarsGlobal Map of Mars ( Modified from Eötvös Lor( Modified from Eötvös Loránd University, 2001 )nd University, 2001 )
  • 6. Geologic Map LegendGeologic Map Legend √ √ √ √ ( Created from GIS tabular data from Scott and Tanaka, 1986 )( Created from GIS tabular data from Scott and Tanaka, 1986 ) √ √
  • 7. Valles Marineris Geologic MapValles Marineris Geologic Map ( Modified from Scott and Tanaka, 1986 )
  • 8. Coprates Chasma Layering andCoprates Chasma Layering and Spur-and-Gully MorphologySpur-and-Gully Morphology b. This close-up is centered at 14.5° South, 55.8° West; Image covers an area of approximately 9.8 km by 17.3 km; North is up ( MOC images courtesy of NASA/JPL/Malin Space Science Systems ) a. Context image b. Central ridge close-up
  • 9. StressStress // Strain RelationshipsStrain Relationships μ = ε1 /ε3 Equation 4.3 Poisson’s ratio, μ, ratio of unit strain perpendicular and parallel to applied stress: Poisson’s ratio describes the ability of a solid to shorten parallel to σ1 without elongation in the σ3 direction, and can vary from 0 (compressible) to 0.5 (incompressible) In the case of ideally viscous (Newtonian) materials, strain rate is related in a linear fashion to applied stress: σ = ηέ Equation 4.4 where η is the viscosity, a material property constant During steady state creep, the stress and strain rate are related in a power law: έ = A exp –(Q/RT)σN Equation 4.5 where T is the absolute temperature; A is a temperature-dependent constant, the frequency factor; Q is a constant, the activation energy for creep; R is the universal gas constant; and N is the stress exponent, typically varying from 1-2 when σ is < 20 MPa, and from 2-4 when 20 < σ < 200 MPa
  • 10. Map of the Deformation Mechanisms of IceMap of the Deformation Mechanisms of Ice As a function of temperature, applied stress, and strain rate ( from Carr, 1996, after Shoji and Higashi, 1978 )
  • 11. Constitutive Relation for IceConstitutive Relation for Ice Glen's Flow Law is widely accepted as the constitutive relation for ice when shear stress acts on its basal plane: where έ is the strain rate; A is a temperature-dependent constant; τb is the basal shear stress; and n is a power law exponent (Glen, 1958) έ = A τb n Equation 4.15  Regards ice as a plastic substance with a yield stress τ of 1 bar (Paterson, 1981)  Value of n generally taken as 3 (Paterson 1981; Johnston, 1981)  Shear strain rate (flow velocity) is lower for colder ice as a function of A  A varies with temperature, and is equal, for example, to 6.8 x 10 -15 s-1 kPa-3 at 273 K, 4.9 x 10-16 at 263 K, 1.7 x 10-16 at 253 K, and 5.1 x 10-17 at 243 K  n varies with applied stress, taking a value of 1 for Newtonian deformation, and 3 for non-Newtonian deformation (Paterson, 1994)  Available evidence indicates that n = 3 for most situations (Russell-Head and Budd, 1979)
  • 12. Deformation of Frozen GroundDeformation of Frozen Ground The total strain in deforming frozen ground is the sum of an instantaneous strain, ε(i) , and a creep strain, ε(c) . The primary creep of frozen ground (and ice) in a state of constant stress can be described by the creep law (Andersland et al., 1978): ε(c) = Kσn tb Equation 4.17 where K, n, and b are temperature-dependent material constants The steady state creep strain is governed by the creep law (Hult, 1966): έ(c) = G(σ, T) Equation 4.18 where έ(c) is the steady state (secondary) creep rate; and the function G(σ,T) is found by plotting the slope dε(c) /dt against the applied stress for various temperatures
  • 13. Temperature Dependence inTemperature Dependence in the Creep Lawthe Creep Law where έc is the creep rate selected for the laboratory experiment - for frozen soils is often taken as 10-5 min-1 (Andersland et al., 1978); σc is the uniaxial stress for the selected creep rate; σc (T) and n(T) are temperature-dependent creep parameters The creep law can be rewritten in the form of a power expression (Hult, 1966; Ladanyi, 1972): έ(c) = έc [σ/σc (T)]n(T) Equation 4.19  The equations for both primary and secondary creep emphasize the temperature-dependence of creep deformation
  • 14. Dependence on Temperature ofDependence on Temperature of CompressiveCompressive Strength for Ice and Various Frozen SoilsStrength for Ice and Various Frozen Soils ( From Andersland et al., 1978; after Sayles, 1966 )
  • 15. Debris-Ice Feature TerminologyDebris-Ice Feature Terminology ( Adapted from Whalley and Azizi, 2003 )
  • 16. Typical Rock Glaciers inTypical Rock Glaciers in Wrangell Mountains, AlaskaWrangell Mountains, Alaska Rock glacier “a” has a single lobe, and rock glacier “b” has a second lobe that appears to have advanced on top of another lobe that advanced at an earlier time ( Adapted from Whalley and Azizi, 2003 )
  • 17. Two Possible Rock-Ice SystemsTwo Possible Rock-Ice Systems in Candor Chasma, Marsin Candor Chasma, Mars Feature “A” resembles a rock glacier, and feature “B” resembles a protalus rampart ( Adapted from Whalley and Azizi, 2003; After Malin et al., 2000 )
  • 18. Enlargements of Candor ChasmaEnlargements of Candor Chasma FeaturesFeatures Feature “A” resembles a rock glacier, and feature “B” resembles a protalus rampart ( Adapted from Whalley and Azizi, 2003; After Malin et al., 2000 ) Enlargement of feature A Enlargement of feature B
  • 19. Mars Orbiter Laser AltimeterMars Orbiter Laser Altimeter (MOLA) Data(MOLA) Data • Polar orbit • Nadir measurements • ±30 cm vertical accuracy • ~150 m spot size • ~330 m along-track spacing (along orbital track) • Good coverage in Valles Marineris region
  • 20. 1/641/64°° Gridded MOLA ElevationGridded MOLA Elevation DataData • 1/64° resolution ≈ 926 m/pixel • Elevation: ±30 cm vertical accuracy • Steepest gradient slope angle • Steepest gradient slope aspect (slope orientation) • Measures of surface roughness: – Curvature (slope of slope) – Surface area ratio (ratio of total surface area to planimetric surface area) • Intermediate products: – Cosine (aspect) – North-South component of slope angle – Local incidence angles • Temperatures
  • 21. 247 Profiles Across Coprates247 Profiles Across Coprates ChasmaChasma Coprates Chasma Trough Wall Cutout marked on this map is the location of the trough wall segment in Figure 6.2. The points marked in green are the starting points for each profile, while the points in red are correspondingly the end points for each profile. From west to east, the two profiles marked in bright red are Coprates Chasma profile number 100 and Coprates Chasma profile number 200, respectively
  • 22. Basic Topographic Architecture ofBasic Topographic Architecture of Coprates ChasmaCoprates Chasma • Extends from 54º to 70º West longitude • 10º to 17º South latitude • ~1,000 km long • Trough trends 100º-104º • Elevations at trough rims range from 0.5 km below datum to 5.5 km above datum – Highest elevations along the segment of the trough extending from 64º to 67º West longitude • Width of trough ranges from 70 km to 125 km • Trough wall heights vary from ~4.5 km to ~10.5 km – Deepest segment of the trough extending from 64º to 67º West longitude
  • 23. Structural Cross-Section ofStructural Cross-Section of Coprates ChasmaCoprates Chasma ( Adapted from Schultz, 1991 )
  • 24. Steepest Gradient Slope Angles andSteepest Gradient Slope Angles and AspectsAspects  Arrow on trough wall points in direction of steepest gradient  Slope angle is calculated in this direction  Slope aspect is the horizontal direction (bearing) in which the arrow points
  • 25. Topographic Profiling RulesTopographic Profiling Rules 1) The trough rim, coming in either direction (~north or ~south) is the first point steeper than 5° where it and the next 14 points (15 points total) average > 8.75° 2) Points selected for analysis must: a) Be located between the rim and the first point at which elevation is <= rim elevation minus 50% of the difference between the rim elevation at that side of the trough (north or south) and the absolute lowest elevation anywhere along the profile (inclusive) b) Have slope aspects within +/- 60° (non-inclusive) of profile trend (for most Coprates profiles, ~194° trend coming from north, correspondingly ~14° trend coming from south) c) Have slope angles > 5° 3) Each of the 5 topographic parameters (elevation, slope angle, slope aspect, curvature, surface area ratio) is averaged in a "selective average" over the wall segment extracted according to 2) as follows: a) The sum of values of the parameter at all points satisfying 2) rules b) The count of points satisfying 2) rules c) a) divided by b) for north and south trough walls, respectively 4) Going downslope, find the first 5 points averaging < 3.7º, last of the 5 is the trough wall bottom
  • 26. Valid Points for Analysis AlongValid Points for Analysis Along Coprates Chasma Profile NumberCoprates Chasma Profile Number 200200  Vertical exaggeration = 6x  Profile aspect = 187.2º (North wall) / 7.2º (South wall)
  • 27. Cryosphere and Thermal EquationsCryosphere and Thermal Equations g msmp Q ΤΤ z − Κ=   Equation 3.1   Tms = 64 K cos i + 154 K Equation 6.2 where z is depth, K is the thermal conductivity of the Martian crust, Tmp is the melting point of ground ice, Tms is the (latitude-dependent) mean annual surface temperature, and Qg is the value of the geothermal heat flux. Nominal values cited for Mars are Qg = 30 mW m-2 , K = 2.0 W m-1 K-1 , and Tmp = 252 K (Clifford, 1993) Steady state one-dimensional heat conduction equation: Simplified surface energy balance equation (Equation 6.1): where i is the local incidence angle; assuming an albedo of Ab = 0.25, a thermal conductivity of k = 2.0 W m-1 K-1 , and ignoring the latent heat of CO2 sublimation (L); works well equatorward of approximately 45º north or south latitude
  • 28. Thermal EquationsThermal Equations 4 2 0 cos)1( T dt dm LF z T kiA R S ab εσ=++ ∂ ∂ +− Equation 6.1 i = abs (l - β) Equation 6.3 β = s cos a Equation 6.4 Surface energy balance equation: where S0 is the solar constant at 1 AU, R is the mean distance of Mars from the sun, Ab is the bolometric albedo, i is the local incidence angle of sunlight, k is the thermal conductivity of the regolith, Fa is the downward component of atmospheric radiation, L is the latent heat of CO2 sublimation, m is the mass of CO2 condensate per unit area, ε is the surface emissivity, σ is the Stephan-Boltzmann constant, and T is temperature (Kieffer et al., 1977; Clifford, 1993) Local incidence angle: where i is the local incidence angle, l is latitude, and β is the north-south component of slope North-south component of slope: where β is the north-south component of slope s is slope angle, and a is slope aspect (slope orientation)
  • 29. Temperature vs. Incidence AngleTemperature vs. Incidence Angle
  • 30. Coprates Chasma TemperatureCoprates Chasma Temperature DataData
  • 31. Temperature vs. LongitudeTemperature vs. Longitude Temperature was calculated using Equation 6.2, Equation 6.3, and Equation 6.4
  • 32. Temperature Along CopratesTemperature Along Coprates Chasma Profile Number 200Chasma Profile Number 200  Vertical exaggeration of elevation profile = 5x
  • 33. Calculated Possible Depths to theCalculated Possible Depths to the Base of the Martian CryosphereBase of the Martian Cryosphere ( Adapted from tabular data, Clifford, 1993 ). The thermal model used Equation 3.1, and with the following values for parameters: Minimum: Qg = 45 mW m-2 , K = 1.0 W m-1 K-1 , and Tmp = 210 K; Nominal: Qg = 30 mW m-2 , K = 2.0 W m-1 K-1 , and Tmp = 252 K; Maximum: Qg = 15 mW m-2 , K = 3.0 W m-1 K-1 , and Tmp = 273 K
  • 34. Coprates Chasma Profile Number 200Coprates Chasma Profile Number 200 with Hypothetical Cryospherewith Hypothetical Cryosphere Calculated using Equation 3.1; Nominal values cited for Mars are Qg = 30 mW m-2 , K = 2.0 W m-1 K-1 , and Tmp = 252 K (Clifford, 1993); Tms was calculated using Equation 6.2, Equation 6.3, and Equation 6.4 a. 6x vertical exaggeration b. No vertical exaggeration 3.6 km 2.2 km
  • 35. Coprates Chasma Slope Angle vs.Coprates Chasma Slope Angle vs. Longitude for North and South WallsLongitude for North and South Walls
  • 36. Coprates Chasma Slope AngleCoprates Chasma Slope Angle DifferencesDifferences
  • 37. Coprates Chasma Curvature vs.Coprates Chasma Curvature vs. LongitudeLongitude
  • 38. Coprates Chasma Surface Area RatioCoprates Chasma Surface Area Ratio vs. Longitudevs. Longitude
  • 39. Paired Differences Between NorthPaired Differences Between North and South Wall Dataand South Wall Data
  • 40. Elevations of Coprates ChasmaElevations of Coprates Chasma Floor and Surrounding PlateausFloor and Surrounding Plateaus
  • 41. Coprates Chasma Trough RimCoprates Chasma Trough Rim Elevation vs. LongitudeElevation vs. Longitude
  • 42. Coprates Chasma Trough WallCoprates Chasma Trough Wall Height vs. LongitudeHeight vs. Longitude
  • 43. Coprates Chasma Trough Wall BottomCoprates Chasma Trough Wall Bottom Elevations for North and South WallsElevations for North and South Walls
  • 44. Coprates Chasma Trough Wall BottomCoprates Chasma Trough Wall Bottom ElevationsElevations • There is NO significant difference in elevation between the North and South trough wall bottoms • The place is FLAT!
  • 45. Slope Angle Correlations WithSlope Angle Correlations With Morphological and Structural PatternsMorphological and Structural Patterns Morphologic and structural patterns are from Peulvast et al. (2001) Morphology Key (1) Cornice with smooth talus slope; (2) Cornice with spurs and gullies; (3a) Crest with spurs and gullies on both sides; (3b) Crest with spurs and gullies on one side and smooth talus slope on the other side; Structure Key (4a) Fault; (4b) Conjectured fault; (5a) Normal fault; (5b) Conjectured normal fault
  • 46. Coprates Chasma Trough Wall HeightCoprates Chasma Trough Wall Height vs. Slope Anglevs. Slope Angle ( Results of Schultz, 2002 Superimposed on Results from this Study; Mége and Gatineau, 2003: RMR = 50-70 )
  • 47. ConclusionsConclusions • North walls of Coprates Chasma 1.33º ± 0.49º steeper than South walls • No significant difference in curvature between North walls and South walls • Surface area ratios 0.011 ± 0.004 higher in the North walls than in the South walls • Cryosphere thickness – ~3.7 km in North walls – ~2.3 km in South walls • ~10 K temperature difference • Similarities between walls – Horizontal stratigraphic layers – Spur-and-gully morphology – Apparently similar materials – Geology • Extremely flat trough floor • Tectonic symmetry