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A. GARDEZ, L. BIENNIER, G. SAIDANI, E. HUGO, R. GEORGES and B. R. ROWE MFHT4 Conference | March 30-31 and April 1st, 2011 | Orléans, France
The classification and evolution of a star The Hertzsprung–Russell diagram shows the relationship between the stars' absolute magnitudes or luminosities versus their spectral types or classifications and effective temperatures. THE ASYMPTOTIC GIANT  BRANCH (AGB) STAR 1
Structure of a ABG star Degenerate C/O Core Convective Stellar envelope Pulsations Radiative zone He- and H-burning shells pseudo photosphère H 2 , CO, H 2 O, TiO, SiO,… CN, C 2  , C n H m , SiC, CH, HCN, … 10 30 10 16 10 9  - 10 6 10 5  - 10 2 10 8   3000 1000 100 r(R*) 10 3 5 1 10 -5   T(K) n(cm -3 ) Dust particules Extended circumstellar envelope Dynamical  atmosphere Shock waves Wind acceleration Dynamical atmosphere of ABG stars is the theater of  rich physical and chemical processes. 2
Molecules detected in the circumstellar envelope of AGB stars Olofsson, H. and coll (2005) Σ = The (rough) number of source detected in each species. The CN + C n H m  reactions studied play an important role in the chemistry of these hot environments. 3
The available laboratory kinetics data CN + C 2n H 2  -> products   National Institute of Standards and Technology (NIST) Reactivity ? 4 Vinyl acetylene propylene propadiene 1,3 butadiene
High enthalpy source (HES) Carbon electrode Water cooled shield Carbon electrode Tantalum Jacket Porous carbon rod Thermal shield 5 Hot gas 10 cm Cold gas
Experimental setup Fluorescence photons Photolysis pulse (CN are generated coaxially to the flow tube) Excitation pulse (CN decays were monitored) 7 Cold reservoir  Tungsten grid Precursor injector Buffer/reactant injector  Roots pump Hot flow Flow reactor
Flow temperature map 30% transparent grid Flow tube Nozzle exit Supersonic expansion Subsonic flow Due to the grid, the flow slows down and its temperature increases.  T 0  = 2200 K,  T wall  = 500 K, Argon buffer gas (20 slm). FLUENT 6.3 software 8
High temperature flows 9 non heated tube Radial distance from the nozzle Axial distance from the nozzle Velocity profile (Ar buffer gas) Boundary layer (Here viscous diffusion rate  ~ thermal diffusion rate)
CN radical as temperature probe of the flow Top : experimental LIF spectrum of the B²Σ + ←X²Σ +  transition of the CN radical in a Ar flow (15.8 slm).  Bottom : simulated LIF spectrum of the CN radical at  T rot  = 745 K and  T vib  = 1300 K using the LIFBASE program.  Boltzmann plot of the rotational distribution obtained from the LIF spectrum of the CN radical.  10
Rate constants measurements: Propane + CN as a test reaction [CN] t  = [CN] 0 exp(- k 1st t ) k 1st  =  k 2nd  [C n H m ] 11
Experimental results CN + C 3 H 8  -> products  Rate coefficients for the reaction of CN (X²Σ+) with propane, C 3 H 8  , as a function of temperature.   12
Experimental results CN + C 3 H 6  -> products  Rate coefficients for the reaction of CN (X²Σ+) with propylene, C 3 H 6  , as a function of temperature.   13
Experimental results CN + C 3 H 4  -> products  Rate coefficients for the reaction of CN (X²Σ+) with propadiene, C 3 H 4  , as a function of temperature.   14
Experimental results CN + 1,3-C 4 H 6  -> products  Rate coefficients for the reaction of CN (X²Σ+) with 1,3-butadiene, 1,3-C 4 H 6  , as a function of temperature.   15
Experimental results CN + 1-C 4 H 6  -> products  Rate coefficients for the reaction of CN (X²Σ+) with 1-butyne, 1-C 4 H 6  , as a function of temperature.   16
Experimental results CN + NH 3  -> NH 2  + HCN (ou CNH)  Rate coefficients for the reaction of CN (X²Σ+) with ammoniac, NH 3  , as a function of temperature.   17
Perspectives  ,[object Object],[object Object],[object Object],18
Thank you for your attention. Questions/Answers ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]

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Mfht4 Orleans

  • 1. A. GARDEZ, L. BIENNIER, G. SAIDANI, E. HUGO, R. GEORGES and B. R. ROWE MFHT4 Conference | March 30-31 and April 1st, 2011 | Orléans, France
  • 2. The classification and evolution of a star The Hertzsprung–Russell diagram shows the relationship between the stars' absolute magnitudes or luminosities versus their spectral types or classifications and effective temperatures. THE ASYMPTOTIC GIANT BRANCH (AGB) STAR 1
  • 3. Structure of a ABG star Degenerate C/O Core Convective Stellar envelope Pulsations Radiative zone He- and H-burning shells pseudo photosphère H 2 , CO, H 2 O, TiO, SiO,… CN, C 2 , C n H m , SiC, CH, HCN, … 10 30 10 16 10 9 - 10 6 10 5 - 10 2 10 8 3000 1000 100 r(R*) 10 3 5 1 10 -5 T(K) n(cm -3 ) Dust particules Extended circumstellar envelope Dynamical atmosphere Shock waves Wind acceleration Dynamical atmosphere of ABG stars is the theater of rich physical and chemical processes. 2
  • 4. Molecules detected in the circumstellar envelope of AGB stars Olofsson, H. and coll (2005) Σ = The (rough) number of source detected in each species. The CN + C n H m reactions studied play an important role in the chemistry of these hot environments. 3
  • 5. The available laboratory kinetics data CN + C 2n H 2 -> products National Institute of Standards and Technology (NIST) Reactivity ? 4 Vinyl acetylene propylene propadiene 1,3 butadiene
  • 6. High enthalpy source (HES) Carbon electrode Water cooled shield Carbon electrode Tantalum Jacket Porous carbon rod Thermal shield 5 Hot gas 10 cm Cold gas
  • 7. Experimental setup Fluorescence photons Photolysis pulse (CN are generated coaxially to the flow tube) Excitation pulse (CN decays were monitored) 7 Cold reservoir Tungsten grid Precursor injector Buffer/reactant injector Roots pump Hot flow Flow reactor
  • 8. Flow temperature map 30% transparent grid Flow tube Nozzle exit Supersonic expansion Subsonic flow Due to the grid, the flow slows down and its temperature increases. T 0 = 2200 K, T wall = 500 K, Argon buffer gas (20 slm). FLUENT 6.3 software 8
  • 9. High temperature flows 9 non heated tube Radial distance from the nozzle Axial distance from the nozzle Velocity profile (Ar buffer gas) Boundary layer (Here viscous diffusion rate ~ thermal diffusion rate)
  • 10. CN radical as temperature probe of the flow Top : experimental LIF spectrum of the B²Σ + ←X²Σ + transition of the CN radical in a Ar flow (15.8 slm). Bottom : simulated LIF spectrum of the CN radical at T rot = 745 K and T vib = 1300 K using the LIFBASE program. Boltzmann plot of the rotational distribution obtained from the LIF spectrum of the CN radical. 10
  • 11. Rate constants measurements: Propane + CN as a test reaction [CN] t = [CN] 0 exp(- k 1st t ) k 1st = k 2nd [C n H m ] 11
  • 12. Experimental results CN + C 3 H 8 -> products Rate coefficients for the reaction of CN (X²Σ+) with propane, C 3 H 8 , as a function of temperature. 12
  • 13. Experimental results CN + C 3 H 6 -> products Rate coefficients for the reaction of CN (X²Σ+) with propylene, C 3 H 6 , as a function of temperature. 13
  • 14. Experimental results CN + C 3 H 4 -> products Rate coefficients for the reaction of CN (X²Σ+) with propadiene, C 3 H 4 , as a function of temperature. 14
  • 15. Experimental results CN + 1,3-C 4 H 6 -> products Rate coefficients for the reaction of CN (X²Σ+) with 1,3-butadiene, 1,3-C 4 H 6 , as a function of temperature. 15
  • 16. Experimental results CN + 1-C 4 H 6 -> products Rate coefficients for the reaction of CN (X²Σ+) with 1-butyne, 1-C 4 H 6 , as a function of temperature. 16
  • 17. Experimental results CN + NH 3 -> NH 2 + HCN (ou CNH) Rate coefficients for the reaction of CN (X²Σ+) with ammoniac, NH 3 , as a function of temperature. 17
  • 18.
  • 19.