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Modeling the influence of nuclear spin in the reaction of H 3 + with H 2. Kyle N. Crabtree , Brian A. Tom, and Benjamin J. McCall University of Illinois. Overview. This talk : Modeling p-H 3 + fraction vs p-H 2 fraction to assess nuclear spin dependence of H 3 + + H 2. - PowerPoint PPT Presentation
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Modeling the influence of nuclear spin in the reaction of H3
+ with H2
Modeling the influence of nuclear spin in the reaction of H3
+ with H2
Kyle N. Crabtree, Brian A. Tom, and Benjamin J. McCall
University of Illinois
Kyle N. Crabtree, Brian A. Tom, and Benjamin J. McCall
University of Illinois
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
2
OverviewOverview
This talk: Modeling p-H3
+ fraction vs p-H2 fraction to assess
nuclear spin dependence of H3
+ + H2
Next talk: Spectroscopic studies at 350 K and 135
K
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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MotivationMotivation• Hydrogen- most abundant
element in the Universe
• H3+ is readily formed from
H2
H2 + CR H2+ + CR¶ + e-
H2 + H2+ H3
+ + H
• Spectroscopic observations of H3
+ in astronomy have been used to measure:– Temperature– Density– Ionization rate– Object size– Ionosphere gas velocity
• Hydrogen- most abundant element in the Universe
• H3+ is readily formed from
H2
H2 + CR H2+ + CR¶ + e-
H2 + H2+ H3
+ + H
• Spectroscopic observations of H3
+ in astronomy have been used to measure:– Temperature– Density– Ionization rate– Object size– Ionosphere gas velocity
Astronomer’s periodic table
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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Nuclear spinNuclear spin
• Observed lines: R(1,0), R(1,1)u, and R(1,1)l
• Nonthermal H3+ in space
• To understand the ortho:para H3
+ ratio,the reaction
H3+ + H2 H2 + H3
+, which interconverts the nuclear spin configurations of H3
+ and H2, must be understood
para-H3+ ortho-H3
+
1/2 3/2
For more on astronomy, see TF09, 160 MA, 3:52 pm
For more on astronomy, see TF09, 160 MA, 3:52 pm
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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H3+ + H2 H2 + H3
+H3+ + H2 H2 + H3
+
“identity”
“hop”
H5+
“exchange”
3
1111
6
Branching fractions: Sid, Shop, Sexch
≡ Shop/Sexch (3/6 = 0.5?)Conservation of nuclear spinangular momentum
Strategy: ensure [H2]>>[H3+],
ortho:para H2 ratio constant
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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Mechanism-specific branching fractionsMechanism-specific branching fractions
id
Reactants o-H3+ p-H3
+
o-H3+ + o-H2 1 0
o-H3+ + p-H2 1 0
p-H3+ + o-H2 0 1
p-H3+ + p-H2 0 1
o-H3+ + o-H2 2/3 1/3
o-H3+ + p-H2 0 1
p-H3+ + o-H2 2/3 1/3
p-H3+ + p-H2 0 1
o-H3+ + o-H2 2/3 1/3
o-H3+ + p-H2 2/3 1/3
p-H3+ + o-H2 1/3 2/3
p-H3+ + p-H2 1/3 2/3
id
exch
hop
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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Steady state p-H3+ fractionSteady state p-H3+ fraction
• Write rate equation for p-H3+, assume ONLY H3
+ + H2 rxn:
• Steady state; p3 ≡ [p-H3+]/[H3
+]; p2 ≡ [p-H2]/[H2]
• Divide through by [H3+][H2]:
• Solve; =kH/kE
• Write rate equation for p-H3+, assume ONLY H3
+ + H2 rxn:
• Steady state; p3 ≡ [p-H3+]/[H3
+]; p2 ≡ [p-H2]/[H2]
• Divide through by [H3+][H2]:
• Solve; =kH/kE
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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“High temperature” model“High temperature” model
Spectroscopically measurable
Experimentally controllable
(n-H2,n-H3+)
(p2=0.25, p3=0.5)
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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Three-body reactionsThree-body reactions
• High densities can lead to formation of larger H2n+1
+ clusters
• At lower pressures, can (H5
+)* clusters undergo proton scrambling with H2?
• High densities can lead to formation of larger H2n+1
+ clusters
• At lower pressures, can (H5
+)* clusters undergo proton scrambling with H2?
H3+ + H2 (H5
+)* H3+ + H2
H5+ + H2
+ H2
H3+ + 2H2 (H7
+)*
?
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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H5+ + H2 H2 + H5
+H5+ + H2 H2 + H5
+
“identity”
1111
“hop”
10
“exchange”
10
H7+
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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“3-body high temperature model”“3-body high temperature model”
• 2 = 2-body branching fraction
• 2, 3 = 2, 3-body hop:exchange ratio
• 2 = 2-body branching fraction
• 2, 3 = 2, 3-body hop:exchange ratio
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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Low temperature modelLow temperature model
• High temperature models based on assumption that nuclear spin statistics exclusively determine reaction outcomes
• At low temperatures, some reaction channels are inhibited due to energetic considerations
• High temperature models based on assumption that nuclear spin statistics exclusively determine reaction outcomes
• At low temperatures, some reaction channels are inhibited due to energetic considerations
p-H2; J = 0
o-H2; J = 1
E = 170 K
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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Low temperature modelLow temperature model
Parameter Value(s)
Trot 10-160 K
Tcoll 10-160 K
Sid 0.1-0.9
Shop 0-1
Sexch 0-1
koooo kooop koopo koopp
kopoo kopop koppo koppp
kpooo kpoop kpopo kpopp
kppoo kppop kpppo kpppp
f (T,Sid,)
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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T
160 K
140 K
120 K
100 K
80 K
60 K
40 K
20 K
Low temperature modelLow temperature model
20 June 2011 66th OSU International Symposium on Molecular Spectroscopy
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SummarySummary
• Measure p-H3+ fraction in known p-H2 fraction plasma
• High temperature models– Reaction outcomes governed by nuclear spin statistics
– 2-body model: only H3+ + H2 reaction
– 3-body model: additional scrambling via (H7+)*
• Low temperature model– Only H3
+ + H2 reaction
– Conservation of nuclear spin, energetic considerations– Dependent on T and Sid
• Next talk, application of models to experimental data• More info:
K. N. Crabtree, B. A. Tom, B. J. McCall, J. Chem. Phys. (2011), 134, 194310.
• Measure p-H3+ fraction in known p-H2 fraction plasma
• High temperature models– Reaction outcomes governed by nuclear spin statistics
– 2-body model: only H3+ + H2 reaction
– 3-body model: additional scrambling via (H7+)*
• Low temperature model– Only H3
+ + H2 reaction
– Conservation of nuclear spin, energetic considerations– Dependent on T and Sid
• Next talk, application of models to experimental data• More info:
K. N. Crabtree, B. A. Tom, B. J. McCall, J. Chem. Phys. (2011), 134, 194310.
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