SlideShare a Scribd company logo
1 of 2
Download to read offline
EXPERIMENTAL SIMULATIONS OF RECURRING SLOPE LINEAE FORMATIONS. J. A. Heydenreich1
,
J. C. Dixon1, 2
and V. F. Chevrier1
. 1
Arkansas Center for Space and Planetary Sciences, 332 N. Arkansas Ave, Uni-
versity of Arkansas, Fayetteville, Arkansas 72701, [jaheyden@uark.edu], 2
Dept. of Geological Sciences, 113 Ozark
Hall, University of Arkansas, Fayetteville, Arkansas, 72701.
Introduction: Recurring slope lineae (RSLs) are
dark streaks that appear annually on the martian sur-
face [1]. They are hypothesized to be formed from
liquid brine flowing downslope in the subsurface.
Emerging from bedrock, RSLs occur on steep slopes
during the warm spring-summer months and fade when
the temperatures decrease in the winter. These features
have been identified most commonly in the southern
mid-latitudes facing the equator [1]. A distinguishable
alcove is formed at the head of the RSL, continuing
into a narrow channel and a depositional fan at the
bottom of the feature [3].
The recurring characteristics of RSLs imply that
not only are RSLs dependent on seasonality, but they
could also indicate a possible persistent subsurface
water source. The presence of recurring water could
form suitable, near-surface environments for life [2].
Although RSLs are generally found on steeper slopes,
lower slopes are better candidates to find extant life.
Lower slopes provide a better habitat for organisms or
detritus because they are less likely to be flushed out
from erosion [2].
Methods: In order to replicate RSLs on the martian
surface, experiments were performed in a 0.67 m x
0.51 m wooden flume. Each experimental run used 8.0
kg of martian regolith simulant, JSC Mars-1. The bulk
density of the regolith inside the flume was approxi-
mately 1.02±0.02 g/cm3
.
For each run, 8.0 kg of Mars JSC-1 was weighed
and added to the wooden flume. The flume was set to
the desired height in order to achieve a slope of 10, 20
or 30 degrees. The water source was introduced by
funneling 100 mL of water through tubing to the
flume. The entrance of the flume consists of a copper
pipe centered at the top of the flume, just underneath
the surface of the regolith. These experiments were
conducted at room temperature.
The experiments were also replicated in a freezer
maintained at -20 °C. This temperature is comparable
to those on Mars during the summer months in which
RSLs appear.
Figure 1: Represents the recurring properties of slope lineae.
A shows the dark streaks appearing in Late Summer, fading
in B and C in Early Spring of the following year and then
reappearing that Early Summer in D. Figure produced from
[1].
Figure 2: The experimental apparatus in room tempera-
ture at a slope of 30° showing the flume, copper pipe
entrance and measured water in the lower right.
1773.pdf47th Lunar and Planetary Science Conference (2016)
Results and Discussion: The results from each ex-
periment show channels of varying lengths, along with
aprons and alcoves (Fig. 3). The channel length for the
-20 °C cold room experiments was 34.6±5.7 cm at 10
degrees, 44.5±10.4 cm at 20 degrees and 46.2±6.2 cm
at 30 degrees. The channel length for the room temper-
ature experiments was 24.6±5.5 cm at 10 degrees,
33.3±3.9 cm at 20 degrees and 34.6±6.7 cm at 30 de-
grees (Fig. 4).
The alcove is designated as the location where the
water exits the copper pipe and creates a depression in
the regolith. Alcove lengths averaged 3-5 cm for the
cold room experiments and 3-4 cm for the room tem-
perature experiments at all slopes. The depositional fan
creates an apron at the bottom of the RSL at an average
length of 16-27 cm for the cold room experiments and
4-16 cm for the room temperature experiments on all
slopes. Although the lengths of the channels did not
change drastically, the width of the stream channel
decreased with increasing slope. It has been observed
that channel widths decrease as slope increases [1].
Thinner channels were noticeable with the highest
slope at 30 degrees.
The maximum height of the sediment deposition at
the base of the channel was also observed. The termi-
nal maximum height increased as the slope increased.
The maximum height averaged between 0.5-1.2 cm in
the cold room and 0.9-1.6 cm at room temperature.
There appears to be a distinction in RSL character-
istics between the cold room and room temperature
experiments. In the cold room experiments, channel,
alcove and apron lengths all tend to be longer than
those associated with the room temperature experi-
ments. The channels of the cold room RSLs are also
generally wider than those of the room temperature
experiments (Fig. 4). However, the heights of the ter-
minal lobes are higher in the room temperature envi-
ronment than the cold room environment.
Future work will test additional slopes in order to
better mimic the slopes associated with RSL for-
mation. Additionally, future experiments will utilize
water with viscosities that are more similar to possible
brines found on Mars.
Conclusion: There was no significant difference in
the total channel, apron and alcove lengths at the vary-
ing slopes (10, 20, and 30 degrees). There was a signif-
icant difference of the channel attributes between the
cold room and room temperature environments. The
width of the channels did appear to decrease with in-
creasing slope. The maximum height of the terminal
lobes of the channel increased in elevation as the slope
increased in both environments. Further experiments
will include additional slopes and different types of
martian analog regolith.
References: [1] McEwen, A. S. et al. (2001) Sci-
ence 333, 740. [2] Stillman, D. E. et al. (2014) Icarus,
233, 328-341. [3] Dickson, J. L. et al. (2007) Icarus,
188, 315-323.
0
5
10
15
20
25
30
35
40
45
50
Alcove Length
(cm)
Total Channel
Length (cm)
Apron Length
(cm)
Max Width
(cm)
Length(cm)
Channel Attributes
Cold Room Experiments
10 Cold
10 Room
20 Cold
20 Room
30 Cold
30 Room
Figure 4: Average lengths (in cm) for each of four
channel attributes (alcove, total length, apron and max
width). Channel attributes correlate with lengths in Fig.
3. Measurements are averaged over five runs for each
slope at 10, 20 and 30 degrees for the cold room and
room temperature experiments.
Figure 3: Gully formation following RSL simulation
conducted with water at a slope of 10 degrees. The al-
cove, total channel length and apron are labeled.
1773.pdf47th Lunar and Planetary Science Conference (2016)

More Related Content

What's hot

Abstractions of precipitation ppt
Abstractions of precipitation pptAbstractions of precipitation ppt
Abstractions of precipitation pptpradeepkumawat4142
 
PPt on Factors affecting evaporation by Prateek
 PPt on Factors affecting evaporation by Prateek PPt on Factors affecting evaporation by Prateek
PPt on Factors affecting evaporation by PrateekPrateek Badola
 
Theory of evaporation
Theory of evaporationTheory of evaporation
Theory of evaporationDaya Madugula
 
Empirical Analysis of Borehole Temperatures
Empirical Analysis of Borehole TemperaturesEmpirical Analysis of Borehole Temperatures
Empirical Analysis of Borehole TemperaturesStephen C. Gronow
 
Factors affecting the rate of evaporation
Factors affecting the rate of evaporationFactors affecting the rate of evaporation
Factors affecting the rate of evaporationdhaneshtandan
 
New evidence for surface water ice in small-scale cold traps and in three lar...
New evidence for surface water ice in small-scale cold traps and in three lar...New evidence for surface water ice in small-scale cold traps and in three lar...
New evidence for surface water ice in small-scale cold traps and in three lar...Sérgio Sacani
 
EGU 2014 Research Abstract
EGU 2014 Research AbstractEGU 2014 Research Abstract
EGU 2014 Research AbstractMaria Blumstock
 
Thermally anomalous features in the subsurface of Enceladus’s south polar ter...
Thermally anomalous features in the subsurface of Enceladus’s south polar ter...Thermally anomalous features in the subsurface of Enceladus’s south polar ter...
Thermally anomalous features in the subsurface of Enceladus’s south polar ter...Sérgio Sacani
 
Team CO2 - Estimating Seismic Velocities and Attenuations of CO2 Saturated Sa...
Team CO2 - Estimating Seismic Velocities and Attenuations of CO2 Saturated Sa...Team CO2 - Estimating Seismic Velocities and Attenuations of CO2 Saturated Sa...
Team CO2 - Estimating Seismic Velocities and Attenuations of CO2 Saturated Sa...finite_parallel
 
Chapter 3
Chapter 3Chapter 3
Chapter 3ECRD IN
 
Air pollution and meteorology
Air pollution and meteorologyAir pollution and meteorology
Air pollution and meteorologyECRD2015
 
Marine isotope stages short doc
Marine isotope stages short docMarine isotope stages short doc
Marine isotope stages short docJGGOKULAKRISHNAN
 
Phes ch17 Atmosphere
Phes ch17 AtmospherePhes ch17 Atmosphere
Phes ch17 Atmospherewindyridge
 

What's hot (20)

Abstractions of precipitation ppt
Abstractions of precipitation pptAbstractions of precipitation ppt
Abstractions of precipitation ppt
 
Meteorology
MeteorologyMeteorology
Meteorology
 
PPt on Factors affecting evaporation by Prateek
 PPt on Factors affecting evaporation by Prateek PPt on Factors affecting evaporation by Prateek
PPt on Factors affecting evaporation by Prateek
 
Poster for BIOS
Poster for BIOSPoster for BIOS
Poster for BIOS
 
Theory of evaporation
Theory of evaporationTheory of evaporation
Theory of evaporation
 
Empirical Analysis of Borehole Temperatures
Empirical Analysis of Borehole TemperaturesEmpirical Analysis of Borehole Temperatures
Empirical Analysis of Borehole Temperatures
 
Unit 2 part 1
Unit 2   part 1Unit 2   part 1
Unit 2 part 1
 
Factors affecting the rate of evaporation
Factors affecting the rate of evaporationFactors affecting the rate of evaporation
Factors affecting the rate of evaporation
 
New evidence for surface water ice in small-scale cold traps and in three lar...
New evidence for surface water ice in small-scale cold traps and in three lar...New evidence for surface water ice in small-scale cold traps and in three lar...
New evidence for surface water ice in small-scale cold traps and in three lar...
 
WOIMSA_conference
WOIMSA_conferenceWOIMSA_conference
WOIMSA_conference
 
Air Temperature & Pressure
Air Temperature & PressureAir Temperature & Pressure
Air Temperature & Pressure
 
EGU 2014 Research Abstract
EGU 2014 Research AbstractEGU 2014 Research Abstract
EGU 2014 Research Abstract
 
Thermally anomalous features in the subsurface of Enceladus’s south polar ter...
Thermally anomalous features in the subsurface of Enceladus’s south polar ter...Thermally anomalous features in the subsurface of Enceladus’s south polar ter...
Thermally anomalous features in the subsurface of Enceladus’s south polar ter...
 
Evaporation (1)
Evaporation (1)Evaporation (1)
Evaporation (1)
 
Team CO2 - Estimating Seismic Velocities and Attenuations of CO2 Saturated Sa...
Team CO2 - Estimating Seismic Velocities and Attenuations of CO2 Saturated Sa...Team CO2 - Estimating Seismic Velocities and Attenuations of CO2 Saturated Sa...
Team CO2 - Estimating Seismic Velocities and Attenuations of CO2 Saturated Sa...
 
Chapter 3
Chapter 3Chapter 3
Chapter 3
 
Air pollution and meteorology
Air pollution and meteorologyAir pollution and meteorology
Air pollution and meteorology
 
Marine isotope stages short doc
Marine isotope stages short docMarine isotope stages short doc
Marine isotope stages short doc
 
Evaluating nitrogen export
Evaluating nitrogen exportEvaluating nitrogen export
Evaluating nitrogen export
 
Phes ch17 Atmosphere
Phes ch17 AtmospherePhes ch17 Atmosphere
Phes ch17 Atmosphere
 

Similar to 1773

Micro cold traps on the Moon
Micro cold traps on the MoonMicro cold traps on the Moon
Micro cold traps on the MoonSérgio Sacani
 
Direct Observation of Subtropical Mode Water in the Western North Atlantic Ocean
Direct Observation of Subtropical Mode Water in the Western North Atlantic OceanDirect Observation of Subtropical Mode Water in the Western North Atlantic Ocean
Direct Observation of Subtropical Mode Water in the Western North Atlantic OceanDavid Fratantoni
 
Direct Observation of Subtropical Mode Water in the Western North Atlantic Ocean
Direct Observation of Subtropical Mode Water in the Western North Atlantic OceanDirect Observation of Subtropical Mode Water in the Western North Atlantic Ocean
Direct Observation of Subtropical Mode Water in the Western North Atlantic OceanDavid Fratantoni
 
Thermohaline Circulation & Climate Change
Thermohaline Circulation & Climate ChangeThermohaline Circulation & Climate Change
Thermohaline Circulation & Climate ChangeArulalan T
 
JWST molecular mapping and characterization of Enceladus’ water plume feeding...
JWST molecular mapping and characterization of Enceladus’ water plume feeding...JWST molecular mapping and characterization of Enceladus’ water plume feeding...
JWST molecular mapping and characterization of Enceladus’ water plume feeding...Sérgio Sacani
 
Weather basics
Weather basicsWeather basics
Weather basicsowenfidler
 
Deep Ocean Circulation (with presenter notes)
Deep Ocean Circulation (with presenter notes)Deep Ocean Circulation (with presenter notes)
Deep Ocean Circulation (with presenter notes)Andreas Schmittner
 
Chapt 6 water & ocean structure
Chapt 6 water & ocean structureChapt 6 water & ocean structure
Chapt 6 water & ocean structureSerena Moon
 
Planetary Vacuums, Atmospheres, & Life
Planetary Vacuums, Atmospheres, & LifePlanetary Vacuums, Atmospheres, & Life
Planetary Vacuums, Atmospheres, & LifePaul H. Carr
 

Similar to 1773 (20)

1240
12401240
1240
 
LPSC_RSL_2016
LPSC_RSL_2016LPSC_RSL_2016
LPSC_RSL_2016
 
Marine bio pp#2,3 2017
Marine bio pp#2,3 2017Marine bio pp#2,3 2017
Marine bio pp#2,3 2017
 
Micro cold traps on the Moon
Micro cold traps on the MoonMicro cold traps on the Moon
Micro cold traps on the Moon
 
Colloquium given at NASA/JPL
Colloquium given at NASA/JPLColloquium given at NASA/JPL
Colloquium given at NASA/JPL
 
Lithosphere
LithosphereLithosphere
Lithosphere
 
Direct Observation of Subtropical Mode Water in the Western North Atlantic Ocean
Direct Observation of Subtropical Mode Water in the Western North Atlantic OceanDirect Observation of Subtropical Mode Water in the Western North Atlantic Ocean
Direct Observation of Subtropical Mode Water in the Western North Atlantic Ocean
 
Direct Observation of Subtropical Mode Water in the Western North Atlantic Ocean
Direct Observation of Subtropical Mode Water in the Western North Atlantic OceanDirect Observation of Subtropical Mode Water in the Western North Atlantic Ocean
Direct Observation of Subtropical Mode Water in the Western North Atlantic Ocean
 
Thermohaline Circulation & Climate Change
Thermohaline Circulation & Climate ChangeThermohaline Circulation & Climate Change
Thermohaline Circulation & Climate Change
 
JWST molecular mapping and characterization of Enceladus’ water plume feeding...
JWST molecular mapping and characterization of Enceladus’ water plume feeding...JWST molecular mapping and characterization of Enceladus’ water plume feeding...
JWST molecular mapping and characterization of Enceladus’ water plume feeding...
 
Ocean properties
Ocean propertiesOcean properties
Ocean properties
 
Weather basics
Weather basicsWeather basics
Weather basics
 
G0372036039
G0372036039G0372036039
G0372036039
 
Deep Ocean Circulation (with presenter notes)
Deep Ocean Circulation (with presenter notes)Deep Ocean Circulation (with presenter notes)
Deep Ocean Circulation (with presenter notes)
 
Poster svalbard 2007
Poster svalbard 2007Poster svalbard 2007
Poster svalbard 2007
 
Lecture 5
Lecture 5Lecture 5
Lecture 5
 
RCEC Email 4.9.03
RCEC Email 4.9.03RCEC Email 4.9.03
RCEC Email 4.9.03
 
Chapt 6 water & ocean structure
Chapt 6 water & ocean structureChapt 6 water & ocean structure
Chapt 6 water & ocean structure
 
Planetary Vacuums, Atmospheres, & Life
Planetary Vacuums, Atmospheres, & LifePlanetary Vacuums, Atmospheres, & Life
Planetary Vacuums, Atmospheres, & Life
 
Annual watercycle
Annual watercycleAnnual watercycle
Annual watercycle
 

1773

  • 1. EXPERIMENTAL SIMULATIONS OF RECURRING SLOPE LINEAE FORMATIONS. J. A. Heydenreich1 , J. C. Dixon1, 2 and V. F. Chevrier1 . 1 Arkansas Center for Space and Planetary Sciences, 332 N. Arkansas Ave, Uni- versity of Arkansas, Fayetteville, Arkansas 72701, [jaheyden@uark.edu], 2 Dept. of Geological Sciences, 113 Ozark Hall, University of Arkansas, Fayetteville, Arkansas, 72701. Introduction: Recurring slope lineae (RSLs) are dark streaks that appear annually on the martian sur- face [1]. They are hypothesized to be formed from liquid brine flowing downslope in the subsurface. Emerging from bedrock, RSLs occur on steep slopes during the warm spring-summer months and fade when the temperatures decrease in the winter. These features have been identified most commonly in the southern mid-latitudes facing the equator [1]. A distinguishable alcove is formed at the head of the RSL, continuing into a narrow channel and a depositional fan at the bottom of the feature [3]. The recurring characteristics of RSLs imply that not only are RSLs dependent on seasonality, but they could also indicate a possible persistent subsurface water source. The presence of recurring water could form suitable, near-surface environments for life [2]. Although RSLs are generally found on steeper slopes, lower slopes are better candidates to find extant life. Lower slopes provide a better habitat for organisms or detritus because they are less likely to be flushed out from erosion [2]. Methods: In order to replicate RSLs on the martian surface, experiments were performed in a 0.67 m x 0.51 m wooden flume. Each experimental run used 8.0 kg of martian regolith simulant, JSC Mars-1. The bulk density of the regolith inside the flume was approxi- mately 1.02±0.02 g/cm3 . For each run, 8.0 kg of Mars JSC-1 was weighed and added to the wooden flume. The flume was set to the desired height in order to achieve a slope of 10, 20 or 30 degrees. The water source was introduced by funneling 100 mL of water through tubing to the flume. The entrance of the flume consists of a copper pipe centered at the top of the flume, just underneath the surface of the regolith. These experiments were conducted at room temperature. The experiments were also replicated in a freezer maintained at -20 °C. This temperature is comparable to those on Mars during the summer months in which RSLs appear. Figure 1: Represents the recurring properties of slope lineae. A shows the dark streaks appearing in Late Summer, fading in B and C in Early Spring of the following year and then reappearing that Early Summer in D. Figure produced from [1]. Figure 2: The experimental apparatus in room tempera- ture at a slope of 30° showing the flume, copper pipe entrance and measured water in the lower right. 1773.pdf47th Lunar and Planetary Science Conference (2016)
  • 2. Results and Discussion: The results from each ex- periment show channels of varying lengths, along with aprons and alcoves (Fig. 3). The channel length for the -20 °C cold room experiments was 34.6±5.7 cm at 10 degrees, 44.5±10.4 cm at 20 degrees and 46.2±6.2 cm at 30 degrees. The channel length for the room temper- ature experiments was 24.6±5.5 cm at 10 degrees, 33.3±3.9 cm at 20 degrees and 34.6±6.7 cm at 30 de- grees (Fig. 4). The alcove is designated as the location where the water exits the copper pipe and creates a depression in the regolith. Alcove lengths averaged 3-5 cm for the cold room experiments and 3-4 cm for the room tem- perature experiments at all slopes. The depositional fan creates an apron at the bottom of the RSL at an average length of 16-27 cm for the cold room experiments and 4-16 cm for the room temperature experiments on all slopes. Although the lengths of the channels did not change drastically, the width of the stream channel decreased with increasing slope. It has been observed that channel widths decrease as slope increases [1]. Thinner channels were noticeable with the highest slope at 30 degrees. The maximum height of the sediment deposition at the base of the channel was also observed. The termi- nal maximum height increased as the slope increased. The maximum height averaged between 0.5-1.2 cm in the cold room and 0.9-1.6 cm at room temperature. There appears to be a distinction in RSL character- istics between the cold room and room temperature experiments. In the cold room experiments, channel, alcove and apron lengths all tend to be longer than those associated with the room temperature experi- ments. The channels of the cold room RSLs are also generally wider than those of the room temperature experiments (Fig. 4). However, the heights of the ter- minal lobes are higher in the room temperature envi- ronment than the cold room environment. Future work will test additional slopes in order to better mimic the slopes associated with RSL for- mation. Additionally, future experiments will utilize water with viscosities that are more similar to possible brines found on Mars. Conclusion: There was no significant difference in the total channel, apron and alcove lengths at the vary- ing slopes (10, 20, and 30 degrees). There was a signif- icant difference of the channel attributes between the cold room and room temperature environments. The width of the channels did appear to decrease with in- creasing slope. The maximum height of the terminal lobes of the channel increased in elevation as the slope increased in both environments. Further experiments will include additional slopes and different types of martian analog regolith. References: [1] McEwen, A. S. et al. (2001) Sci- ence 333, 740. [2] Stillman, D. E. et al. (2014) Icarus, 233, 328-341. [3] Dickson, J. L. et al. (2007) Icarus, 188, 315-323. 0 5 10 15 20 25 30 35 40 45 50 Alcove Length (cm) Total Channel Length (cm) Apron Length (cm) Max Width (cm) Length(cm) Channel Attributes Cold Room Experiments 10 Cold 10 Room 20 Cold 20 Room 30 Cold 30 Room Figure 4: Average lengths (in cm) for each of four channel attributes (alcove, total length, apron and max width). Channel attributes correlate with lengths in Fig. 3. Measurements are averaged over five runs for each slope at 10, 20 and 30 degrees for the cold room and room temperature experiments. Figure 3: Gully formation following RSL simulation conducted with water at a slope of 10 degrees. The al- cove, total channel length and apron are labeled. 1773.pdf47th Lunar and Planetary Science Conference (2016)