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PAMPRE and the Chemistry of Neutral Species in Titan's Upper Atmosphere

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HAL Id: insu-01336838

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Submitted on 24 Jun 2016

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PAMPRE and the Chemistry of Neutral Species in Titan’s Upper Atmosphere

David Dubois, Nathalie Carrasco, Sarah Tigrine, Ludovic Vettier, Guy Cernogora

To cite this version:

David Dubois, Nathalie Carrasco, Sarah Tigrine, Ludovic Vettier, Guy Cernogora. PAMPRE and the Chemistry of Neutral Species in Titan’s Upper Atmosphere. Exobiologie Jeunes Chercheurs 2015, Nov 2015, Paris, France. 2015. �insu-01336838�

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PAMPRE and the Chemistry of Neutral Species in

Titan’s Upper Atmosphere

D. Dubois, N. Carrasco, S. Tigrine, L. Vettier, G. Cernogora

Université Versailles St-Quentin, UPMC Univ. Paris 06, CNRS, LATMOS, 11 Blvd. d’Alembert, 78280 Guyancourt, France

[1] Abstract

[2] Introduction

[4] Infrared Spectroscopy

[5] Mass Spectrometry

References

[6] Perspectives

A complex atmospheric photochemistry has been revealed in Titan’s

atmosphere by the ongoing Cassini-Huygens mission. Its

composition mainly made out of N

2

-CH

4

leads to ionization and

photo-dissociative processes that eventually form solid organic aerosols

called tholins. Tholins are assumed to be formed in the ionosphere,

where they coexist with the gas phase, in an ionic and neutral medium.

The PAMPRE set-up aims at simulating the reactivity and production of

solid aerosols in Titan’s ionospheric conditions through heterogeneous

chemistry in a radiofrequency-induced plasma.

In this study, our aim was to accumulate gas products in an N

2

-CH

4

(90-10%) mixture using a cold trap to retain the products. These were

then released after end of cooling and analyzed with infrared

spectroscopy and mass spectrometry in order to better understand the

chemical reactivity at work.

Fig. 9. (a) Ion mass spectra measured in an RF plasma (adapted from

Mutsukura, 2001)

(b) Qualitative comparison of positive ions in an RF plasma and in

Titan’s ionosphere (Carrasco et al., 2012)

Ø Cable, M., Hörst, S., Hodyss, R., Beauchamp, P., Smith, M., Willis, P., 2011. Titan

Tholins: Simulating Titan Organic Chemistry in the Cassini-Huygens Era, Chem. Rev., 112, 1882-1909.

Ø Carrasco, N., Gautier, T., Es-sebbar, E., Pernot, P., Cernogora, G., 2012. Volatile

products controlling Titan’s tholins production. Icarus 219, 230-240.

Ø Mandt, K., et al., 2012. Ion densities and composition of Titan’s upper atmosphere,

JGR, 117, E10006.

Ø Mutsukura, N., 2001. Deposition of diamondlike carbon film and mass spectrometry

measurement in CH4/N2 RF plasma. Plasma Chem. Plasma Process. 21, 265–277.

Ø Szopa, C., Cernogora, G., Boufendi, L., Correia, J-J., Coll, P., 2006. PAMPRE: A dusty

plasma experiment for Titan's tholins production and study. Planetary and Space Science, 54, 394-404.

Fig. 1. The intense photochemistry leading up to

the formation of aerosols that make up the hazy layers on Titan. Image credit: ESA/ATG medialab

Fig. 2. The PAMPRE RF plasma experiment

(Szopa et al., 2006)

[3] The experiment

Fig. 4. The cryogenic trap system

2015

o The cryogenic trap

was set at a

temperature of Tº=

100 K in order to try

and trap as many

products as possible

1000 1500 2000 2500 3000 3500 4000 0 0.02 0.04 0.06 0.08 0.1 0.12 Wav e n u m b e r ( c m - 1) Ab so rb a n ce

I n f r ar e d ab sor b an c e of t h e r e l e ase d gas p r o d u c t s af t e r 10m n an d 24h of w ar m i n g

t=10mn of warming t=24h of warming 1500 2000 2500 3000 3500 4000 0 0.02 0.04 0.06 0.08 0.1 0.12 Wav e n u m b e r ( c m - 1) Abs o rb a n c e R e p r o d u c i b i l i ty i n i n f r ar e d ab sor b an c e of t h e gas p r o d u c t s Gas products released after 24h (1st run)

Gas products released after 21h (2nd run)

0 150 300 450 600 750 900 1050 1200 1350 1500 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 T i m e ( m n ) Pr e ss u re (m b a r)

P r e ssu r e e v ol u t i on of t h e r e l e ase d gas p r o d u c t s d u r i n g w ar m i n g f or 21h

0.38 0.70 0.74 0.93 1.28 1.60 1.84 Gas product pressures

o In light of this study of neutral species, the next step

will be to analyze positive and negative ions by

secondary ion mass spectrometry coupled with the

reactor.

Fig. 6. Infrared absorption of the gas products released after

cryogenic trap, with zoom centered at 4000 cm-1, compared

with the GEISA spectroscopy database

Fig. 7. Test of reproducibility

o Data provided by

the INMS

instrument

onboard Cassini

showed the

prevalence of ion

chemistry leading

to the formation

of the tholins

(Mandt et al.,

2012).

Fig. 5. Pressure evolution of the gas

products released after end of cooling

Fig. 3. Background mass spectrum

0 10 20 30 40 50 60 70 80 90 100 1 2 3 4 5 6 7x 10 −10 M ass ( am u ) Io n c u rr e n t [A ] B ac k gr ou n d N 2- C H 4 m ass sp e c t r u m Background 0 10 20 30 40 50 60 70 80 90 100 10−14 10−13 10−12 10−11 10−10 10−9 10−8 M ass ( am u ) Io n c u rr e n t [A ] M ass sp e c t r a of gas p r o d u c t s i n an N 2- C H 4 m i x t u r e

Products released after 7mn (P=0.38 mbar) Products released after 32mn (P=0.70 mbar)

0 10 20 30 40 50 60 70 80 90 100 10−14 10−13 10−12 10−11 10−10 10−9 10−8 M a s s ( a m u ) Io n c u rr e n t [A ] M a s s s p e c t r a o f g a s p r o d u c t s i n a n N 2 - C H 4 m i x t u r e

Products released after 76mn (P=0.74 mbar) Products released after 125mn (P=0.93 mbar)

0 10 20 30 40 50 60 70 80 90 100 10−14 10−13 10−12 10−11 10−10 10−9 10−8 M as s ( am u ) Io n c u rr e n t [A ] M as s s p e c t r a of gas p r o d u c t s i n an N 2- C H 4 m i x t u r e

Products released after 190mn (P=1.28 mbar) Products released after 300mn (P=1.60 mbar)

0 10 20 30 40 50 60 70 80 90 100 10−14 10−13 10−12 10−11 10−10 10−9 10−8 M as s ( am u ) Io n c u rr e n t [A ] M as s s p e c t r u m of al l gas p r o d u c t s i n an N 2- C H 4 m i x t u r e

Products released after 21h (P=1.84 mbar)

Fig. 8. Gas products released after 32mn (a), 125mn (b), 300mn (c) and 21h

(d). The final pressure of gas products attained here is 1.84 mbar. For the first 32mn, C1 and C2 molecules are already well present. C3 and C4

compounds appear after 76mn. C5, C6 and higher mass molecules are detectable back at room temperature, at the end of our experiment.

(a)

(b)

(c)

(d)

NH3 HCN N2 CH4 C6H6 C4H6 C6H6 HCN C1 C2 C4 C5 C6 C7 3500 3600 3700 3800 3900 4000 4100 4200 4300 4400 0 0.02 0.04 0.06 0.08 0.1 0.12 Wav e n u m b e r ( c m - 1) Ab so rb a n ce t=10mn of warming t=24h of warming HCN HCN

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