new cordier1, d., barnes2, j. w. and ferreira3, a.g.m. · 2013. 3. 6. · the results of simulatons...

1
Cordier Cordier 1 1 , D., Barnes , D., Barnes 2 2 , J. W. and Ferreira , J. W. and Ferreira 3 3 , A.G.M. , A.G.M. 1 Instut UTINAM, CNRS, UMR 6213, Université de Franche-Comté, 41bis, avenue de l’Observatoire, 25 000 Besançon, France Instut UTINAM, CNRS, UMR 6213, Université de Franche-Comté, 41bis, avenue de l’Observatoire, 25 000 Besançon, France 2 Department of Physics, University of Idaho, Engineering-Physics Building, Moscow, ID 83844, USA 3 Departamento de Engenharia Quimica, Universidade de Coimbra, Coimbra 3030-290, Portugal Departamento de Engenharia Quimica, Universidade de Coimbra, Coimbra 3030-290, Portugal ABSTRACT ABSTRACT Titan, the main satellite of Saturn, seems to have an active cycle of methane in its troposphere. Among other evidences of a mechanism of evaporation at work on the ground, dry lakebeds have been discovered dry lakebeds have been discovered. Recently, CASSINI infrared observations of these empty lakes have revealed a surface composition poor in water ice compared to that of the surrounding terrains; suggesting the existence of organic evaporites deposits. The chemical composition of these possible evaporites is unknown. In this work, we propose a study of evaporites composition using a model of organic solids dissolution and of the solvent evaporation. Our results suggest the possibility of large abundances of butane butane and acetylene acetylene in the lake evaporites. But, due to uncertainties of the employed theory, these determinations have to be confirmed by laboratory experiments. I- Introducon I- Introducon Since the eightes, the existence of liquid hydrocarbons at the surface of Titan has been suspected (see for instance Sagan & Dermot, 1982). Thanks to the Cassini orbiter RADAR system, dark paterns were observed in the north polar region of the main satellite of Saturn (Stofan et al., 2007). These features, presented a very low refectvity in the RADAR wave lengths domain and a morphology similar to Earth's lakes one. Consequently, they have been interpreted as hydrocarbon lakes, this interpretaton has been reinforced by the observaton of a specular refecton of sunlight through the 5-μm window (Stephan et al., 2010). Such lakes have also been detected in the south hemisphere polar area (Turtle et al., 2009), but they show a smaller surface coverage. Already, during the frst RADAR lakes detecton, the presence of features that look like dry lakebeds have been notced. A strong correlaton between RADAR dry lakebeds and surface patches bright at 5-μm has been found by Barnes et al . (2011). This brightness associated to high refectvity in the 2.8−μm window relatve to the 2.7−μm window, seems to be characteristc of very low water ice abundance relatve to the rest of Titan (Barnes et al. 2009, Barnes et al. 2011). The neighbouring terrains having a diferent aspect in infrared VIMS observatons. In summary, all of this suggests the formaton of an evaporitc layer of organic mater in the Titan's liquid empty lakebeds. Other observatons speak in favor of the existence of evaporaton processes from lakes. For instance, evidences for actve shoreline processes have been reported (Wall et al. 2010, Barnes et al. 2009a). On the theoretcal side, several authors have developed models that take into account a possible evaporaton of lakes (Mitri et al. 2007, Tokano 2009). The queston of the compositon of potental lakebeds evaporites is stll widely opened; the present work is dedicated to what can be answered with the help of the solubility models including evaporaton of methane and ethane. Contact: [email protected] References References Sagan & Dermott, Nature, 300, 731, (1982). Stofan, et al. Nature, 445, 61, (2007). Stephan, et al, GRL, 37, L07104 (2010). Turtle, et al, GRL, L02204 (2009). Barnes, et al. Icarus, 216, 136 (2011).Barnes, et al, Icarus, 201, 217 (2009). Wall, et al, GRL, 37, L05202 (2010). Mitri, et al, Icarus, 186, 385 (2007). Tokano, Astrobiology, 9, 147 (2009). Brown, et al. Nature, 454, 607 (2008). Dubouloz, et al, Icarus, 82, 81 (1989). Cordier, et al., ApJL, L128 (2009). Cordier, et al., PSS, 61, 99 (2012). II- The Model II- The Model We consider a lake as a liquid phase with only three volatle compounds: methane, ethane and nitrogen; the roles of argon and carbon monoxyde are neglected. The species which are supposed to dissolved in the methane-ethane mixture are those indicated in Table 1. This inventory comes from photochemichal models, these compounds are in solid state under the thermodynamic conditons of the Titan's surface. Methane and ethane evaporate at respectve evaporaton rates F CH 4 and F C2H6 supposed to be known at each tme t. According to equilibrium models (see for instance Cordier et al. 2009) the abundance of nitrogen is supposed to be of the order of a percent and its evaporaton rate is scaled to the ethane one. The quanttes of CH 4 and C 2 H 6 that evaporates during the tme interval between t and t + Δt are computed and new mole fractons X i (new) of solutes are derived. These updated values are compared to the mole fractons at saturaton ( X i sat ) which are provided by the equaton (1) (1) If X i (new) > X i sat , then we fx X i (new) = X i sat , the exceeding material is assumed to become solid instantaneously at the lake bed, the other mole fractons are adjusted to insure Σ i X i = 1. Taking into consideraton the mater precipatng, the compositon of the evaporitc layer ( X i evap ) at tme tt can be easily calculated. The procedure is repeated untl all the inital quantty of solvent is gone. For the sake of simplicity, we frst consider here an ideal soluton, i.e. a soluton for which the actvity coefficients Γ i equal the unity for all species. The calculaton is conducted over the evaporaton tme-scale τ CH4+C2H6 , that way a precise knowledge of evaporaton rate F CH4 and F C2H6 is not required. This is a very helpful assumpton as these rates depend on numerous and unknown parameters: temperature diference between lake and atmosphere, actual atmospheric mole fracton of methane and ethane, the speed of wind, etc (Mitri et al. 2007, Tokano 2009). Fig. 1 Fig. 1 This fgure shows, on Titan, the area south to the north-polar sea Ligea Mare. This is a combined VIMS-RADAR view; the VIMS data are color- mapped with R= 5 μm, G= 2 μm, B= 1.3 μm. The zones that appear in orangish/yellowish are interpreted like terrains poor in water ice, suggesting the existence of an organic deposit. The correlation between these zones and the RADAR patterns with the morphology of dry lakebeds is remarkable. Tab. 3 Tab. 3 Notation: x.y(-n)= x.y 10 -n Tab. 2 Tab. 2 Notaton: x.y(-n)= x.y 10 -n Tab. 4 Tab. 4 Notation: x.y(-n)= x.y 10 -n III- The Results III- The Results We have considered two kinds of inital liquid mixtures. On one hand ( type 1 mixture), we chose a mixture with dissolved solids mole fractons scaled to precipitaton rates; forcing HCN, the most abundant species in atmospheric precipitatons having its mole fracton set to its value at saturaton (ideal case). On the other hand ( type 2 mixture), we took a mixture in which all the species had the same abundance, fxed to the smallest mole fracton at saturaton (i.e. that relatve to C 6 H 6 , see Tab. 1). All computatons were performed at temperature T= 90 K, typical of the lakes regions. In Tab. 2, results relevant for an ideal soluton have been gathered. The inital type 1 and 2 mixtures have been considered, both ethane rich (~89% of C 2 H 6 when evaporaton startng) with ~1% of nitrogen to ensure the liquid physical state. While X liq ini quantfes the inital chemical compositon of the soluton, X sol ini represents the abundances of dissolved solids separated from the solvent (i.e. CH 4 , C 2 H 6 and N 2 ), the X evap fn 's are the mole fractons of compounds fnally deposited in the evaporites upper layer; the parameter of enrichment Δ measures the relatve enrichment/empoverichment of a given species in the surface evaporites, compared to the inital compositon of solids. As it can be notced in Tab. 2, the only species undergoing an enrichment in the surface evaporites layer, compared to abundances initally taken into account for the dissolved solids, are butane (C 4 H 10 ) and acetylene (C 2 H 2 ). This behavior can be explained by their high solubilites (i.e. high X i sat 's). The higher X i sat is, the more the quantty of dissolved material is. Consequently the saturaton occurs later during the evaporaton process. If we compare X fn evap obtained for type 1 and type 2 mixtures of solids, we see that evaporite compositon obviously depends on the inital abundances of solutes. Our simulaton clearly shows, in the frame of our current assumptons, that dissoluton in methane/ethane soluton, followed by evaporaton of the solvent, yields to surface evaporite compositon with high abundances of the most soluble species. We stress that identcal parameter of the enrichment Δ is the consequence of a saturaton of solutes that occurs at the very end of the evaporaton. Of course, a solvent of a diferent compositon (e.g. a methane rich one) leads strictly to the same result as here we are making the calculatons by adoptng the ideal soluton hypothesis. The results of simulatons for which the regular soluton Γ i 's (non-ideal soluton) have been gathered in Tab. 3 and Tab. 4, which are respectvely devoted to dissolved solids mixture type 1 and type 2. For each of these types, cases of methane rich and poor solvent are considered. As it can be notced in Tab. 3 and Tab. 4, the general trend remains the same: butane and acetylene, if present in the inital mixture, are the dominant species in the upper evaporite layer. The diference between the results of methane rich and poor are explained by the non-ideality of the soluton: in such a situaton the molecules undergo interactons, this way solvents with diferent compositons are not equivalent. IV- Discussion IV- Discussion We have checked that reasonable variatons in the temperature or in the nitrogen abundance do not alter signifcantly the observed tendency concerning the chemical compositon of possible evaporites. However Eq. (1) is an approximaton of Eq. (2) (2) Unfortunately the ΔC p ’s are not known for the relevant range of temperature and the regular soluton theory (actvity coefficients Γ i calculaton) sufers from uncertaintes (see Cordier et al. 2012), this is why laboratory experiments of dissoluton of organic solids in methane/ethane mixtures are required for an improved understanding of the Titan’s evaporites formaton.

Upload: others

Post on 27-Oct-2020

0 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: New Cordier1, D., Barnes2, J. W. and Ferreira3, A.G.M. · 2013. 3. 6. · The results of simulatons for which the regular soluton Γi's (non-ideal soluton) have been gathered in Tab

CordierCordier11, D., Barnes, D., Barnes22, J. W. and Ferreira, J. W. and Ferreira33, A.G.M., A.G.M.

11 Institut UTINAM, CNRS, UMR 6213, Université de Franche-Comté, 41bis, avenue de l’Observatoire, 25 000 Besançon, France Institut UTINAM, CNRS, UMR 6213, Université de Franche-Comté, 41bis, avenue de l’Observatoire, 25 000 Besançon, France22 Department of Physics, University of Idaho, Engineering-Physics Building, Moscow, ID 83844, USA33 Departamento de Engenharia Quimica, Universidade de Coimbra, Coimbra 3030-290, Portugal Departamento de Engenharia Quimica, Universidade de Coimbra, Coimbra 3030-290, Portugal

ABSTRACTABSTRACT Titan, the main satellite of Saturn, seems to have an active cycle of methane in its troposphere. Among other evidences of a mechanism of evaporation at work on the ground, dry lakebeds have been discovereddry lakebeds have been discovered. Recently, CASSINI infrared observations of these empty lakes have revealed a surface composition poor in water ice compared to that of the surrounding terrains; suggesting the existence of organic evaporites deposits. The chemical composition of these possible evaporites is unknown. In this work, we propose a study of evaporites composition using a model of organic solids dissolution and of the solvent evaporation. Our results suggest the possibility of large abundances of butanebutane and acetyleneacetylene in the lake evaporites. But, due to uncertainties of the employed theory, these determinations have to be confirmed by laboratory experiments.

I- Introduction I- Introduction Since the eightes, the existence of liquid hydrocarbons at the surface of Titan has been suspected (see for instance Sagan & Dermot, 1982). Thanks to the Cassini orbiter RADAR system, dark paterns were observed in the north polar region of the main satellite of Saturn (Stofan et al., 2007). These features, presented a very low refectvity in the RADAR wave lengths domain and a morphology similar to Earth's lakes one. Consequently, they have been interpreted as hydrocarbon lakes, this interpretaton has been reinforced by the observaton of a specular refecton of sunlight through the 5-μm window (Stephan et al., 2010). Such lakes have also been detected in the south hemisphere polar area (Turtle et al., 2009), but they show a smaller surface coverage. Already, during the frst RADAR lakes detecton, the presence of features that look like dry lakebeds have been notced. A strong correlaton between RADAR dry lakebeds and surface patches bright at 5-μm has been found by Barnes et al. (2011). This brightness associated to high refectvity in the 2.8−μm window relatve to the 2.7−μm window, seems to be characteristc of very low water ice abundance relatve to the rest of Titan (Barnes et al. 2009, Barnes et al. 2011). The neighbouring terrains having a diferent aspect in infrared VIMS observatons. In summary, all of this suggests the formaton of an evaporitc layer of organic mater in the Titan's liquid empty lakebeds. Other observatons speak in favor of the existence of evaporaton processes from lakes. For instance, evidences for actve shoreline processes have been reported (Wall et al. 2010, Barnes et al. 2009a). On the theoretcal side, several authors have developed models that take into account a possible evaporaton of lakes (Mitri et al. 2007, Tokano 2009). The queston of the compositon of potental lakebeds evaporites is stll widely opened; the present work is dedicated to what can be answered with the help of the solubility models including evaporaton of methane and ethane.

Contact: [email protected]

References References Sagan & Dermott, Nature, 300, 731, (1982). Stofan, et al. Nature, 445, 61, (2007). Stephan, et al, GRL, 37, L07104 (2010). Turtle, et al, GRL, L02204 (2009). Barnes, et al. Icarus, 216, 136 (2011).Barnes, et al, Icarus, 201, 217 (2009). Wall, et al, GRL, 37, L05202 (2010). Mitri, et al, Icarus, 186, 385 (2007). Tokano, Astrobiology, 9, 147 (2009). Brown, et al. Nature, 454, 607 (2008). Dubouloz, et al, Icarus, 82, 81 (1989). Cordier, et al., ApJL, L128 (2009). Cordier, et al., PSS, 61, 99 (2012).

II- The Model II- The Model We consider a lake as a liquid phase with only three volatle compounds: methane, ethane and nitrogen; the roles of argon and carbon monoxyde are neglected. The species which are supposed to dissolved in the methane-ethane mixture are those indicated in Table 1. This inventory comes from photochemichal models, these compounds are in solid state under the thermodynamic conditons of the Titan's surface. Methane and ethane evaporate at respectve evaporaton rates FCH4

and FC2H6 supposed to be known at each tme t. According to equilibrium models

(see for instance Cordier et al. 2009) the abundance of nitrogen is supposed to be of the order of a percent and its evaporaton rate is scaled to the ethane one.

The quanttes of CH4 and C2H6 that evaporates during the tme interval between t and t + Δt arecomputed and new mole fractons Xi

(new) of solutes are derived. These updated values are compared to the mole fractons at saturaton (Xi

sat) which are provided by the equaton (1)

(1)

If Xi(new) > Xi

sat, then we fx Xi(new) = Xi

sat, the exceeding material is assumed to become solid instantaneously at the lake bed, the other mole fractons are adjusted to insure Σi Xi = 1. Taking into consideraton the mater precipatng, the compositon of the evaporitc layer (Xi

evap) at tme t+Δt can be easily calculated. The procedure is repeated untl all the inital quantty of solvent is gone. For the sake of simplicity, we frst consider here an ideal soluton, i.e. a soluton for which the actvity coefficients Γi equal the unity for all species. The calculaton is conducted over the evaporaton tme-scale τCH4+C2H6, that way a precise knowledge of evaporaton rate FCH4 and FC2H6 is not required. This is a very helpful assumpton as these rates depend on numerous and unknown parameters: temperature diference between lake and atmosphere, actual atmospheric mole fracton of methane and ethane, the speed of wind, etc (Mitri et al. 2007, Tokano 2009).

Fig. 1 Fig. 1 This fgure shows, on Titan, the area south to the north-polar sea Ligea Mare. This is a combined VIMS-RADAR view; the VIMS data are color-mapped with R= 5 μm, G= 2 μm, B= 1.3 μm. The zones that appear in orangish/yellowish are interpreted like terrains poor in water ice, suggesting the existence of an organic deposit. The correlation between these zones and the RADAR patterns with the morphology of dry lakebeds is remarkable.

Tab. 3 Tab. 3 Notation: x.y(-n)= x.y 10-nTab. 2 Tab. 2 Notaton: x.y(-n)= x.y 10-n Tab. 4 Tab. 4 Notation: x.y(-n)= x.y 10-n

III- The Results III- The Results We have considered two kinds of inital liquid mixtures. On one hand (type 1 mixture), we chose a mixture with dissolved solids mole fractons scaled to precipitaton rates; forcing HCN, the most abundant species in atmospheric precipitatons having its mole fracton set to its value at saturaton (ideal case). On the other hand (type 2 mixture), we took a mixture in which all the species had the same abundance, fxed to the smallest mole fracton at saturaton (i.e. that relatve to C6H6, see Tab. 1). All computatons were performed at temperature T= 90 K, typical of the lakes regions.

In Tab. 2, results relevant for an ideal soluton have been gathered. The inital type 1 and 2 mixtures have been considered, both ethane rich (~89% of C2H6 when evaporaton startng) with ~1% of nitrogen to ensure the liquid physical state. While Xliq

ini quantfes the inital chemical compositon of the soluton, Xsolini represents the abundances of dissolved solids separated from the solvent (i.e. CH4, C2H6 and N2), the Xevap

fn's are the mole fractons of compounds fnally deposited in the evaporites upper layer; the parameter of enrichment Δ measures the relatve enrichment/empoverichment of a given species in the surface evaporites, compared to the inital compositon of solids. As it can be notced in Tab. 2, the only species undergoing an enrichment in the surface evaporites layer, compared to abundances initally taken into account for the dissolved solids, are butane (C4H10) and acetylene (C2H2). This behavior can be explained by their high solubilites (i.e. high Xi

sat's). The higher Xisat is, the more the quantty of dissolved material is. Consequently the saturaton occurs later during the evaporaton process. If we compare Xfn

evap obtained for type 1 and type 2 mixtures of solids, we see that evaporite compositon obviously depends on the inital abundances of solutes. Our simulaton clearly shows, in the frame of our current assumptons, that dissoluton in methane/ethane soluton, followed by evaporaton of the solvent, yields to surface evaporite compositon with high abundances of the most soluble species. We stress that identcal parameter of the enrichment Δ is the consequence of a saturaton of solutes that occurs at the very end of the evaporaton. Of course, a solvent of a diferent compositon (e.g. a methane rich one) leads strictly to the same result as here we are making the calculatons by adoptng the ideal soluton hypothesis. The results of simulatons for which the regular soluton Γi's (non-ideal soluton) have been gathered in Tab. 3 and Tab. 4, which are respectvely devoted to dissolved solids mixture type 1 and type 2. For each of these types, cases of methane rich and poor solvent are considered. As it can be notced in Tab. 3 and Tab. 4, the general trend remains the same: butane and acetylene, if present in the inital mixture, are the dominant species in the upper evaporite layer. The diference between the results of methane rich and poor are explained by the non-ideality of the soluton: in such a situaton the molecules undergo interactons, this way solvents with diferent compositons are not equivalent.

IV- Discussion IV- Discussion We have checked that reasonable variatons in the temperature or in the nitrogen abundance do not alter signifcantly the observed tendency concerning the chemical compositon of possible evaporites. However Eq. (1) is an approximaton of Eq. (2)

(2)

Unfortunately the ΔCp’s are not known for the relevant range of temperature and the regular soluton theory (actvity coefficients Γi calculaton) sufers from uncertaintes (see Cordier et al. 2012), this is why laboratory experiments of dissoluton of organic solids in methane/ethane mixtures are required for an improved understanding of the Titan’s evaporites formaton.