N + NO

Gaz phase reaction (type: Bimolecular reactions)  


     
 
Datasheet    T(K) = 10-300   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 10-300
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2013-10-16
k( )
cm3s-1
Details
1.07e-11 N + NO → O + N2
T(K) = 10-300
α = 4.00E-11
β = -2.00E-1
γ = 2.00E+1
F 0 = 1.4
g = 10
Type uncert: lognormal
Method: Reviews and Evaluations
Reference
Origin: Datasheet
Authors:
Volume,Page:
Year:
DOI: -
Download citation:
 
Wennberg, P. O. et al (1994)    T(K) = 213-369   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 213-369
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2016-01-06
k( )
cm3s-1
Details
1.95e-4 N + NO → O + N2
T(K) = 213-369
α = 2.20E-11
β = 0.00E+0
γ = -1.60E+2
F 0 = 0
g = 0
Type uncert: lognormal
Method: Measurements
Description: Flow reactor. Microwave discharge of trace N2 in He and atomic resonance fluorescence using a gas filter scheme.
Reference
Origin: Bibliography
Authors: Wennberg, P. O. et al
Volume,Page: 99, 18839
Year: 1994
DOI: -
Download citation: Bibtex RIS
 
Lee, J. H. et al (1978)    T(K) = 196-370   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 196-370
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2024-10-12
k( )
cm3s-1
Details
2.70e-11 N + NO → O + N2
T(K) = 196-370
α = 2.70E-11
β = 0.00E+0
γ = 0.00E+0
F 0 = 0
g = 0
Type uncert: lognormal
Method: Measurements
Description: Discharge flow-filtered resonance fluorescence (DF-RF) and flash photolysis of N2O-resonance fluorescence (FP-RF).
Reference
Origin: Bibliography
Authors: Lee, J. H. et al
Volume,Page: 69, 3069-3076
Year: 1978
DOI: -
Download citation: Bibtex RIS
 
Gamallo, P. et al (2006)    T(K) = 200-2500   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 200-2500
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2024-10-12
k( )
cm3s-1
Details
3.94e-6 N + NO → O + N2
T(K) = 200-2500
α = 2.15E-11
β = 2.80E-1
γ = -1.31E+2
F 0 = 0
g = 0
Type uncert: lognormal
Method: Calculations
Description: Time-dependent real wave-packet (WP) quantum dynamics rate constants on the 1 3A” and 1 3A’ analytical potential energy surfaces (PES). The 3A” PES is barrierless along the minimum energy path, while the analytical 3A’ excited PES presents an energy barrier of 36.57 kJ mol-1, including zero point energy.
Reference
Origin: Bibliography
Authors: Gamallo, P. et al
Volume,Page: 124, 174303-11
Year: 2006
DOI: -
Download citation: Bibtex RIS
 
Other database : UdFA    T(K) = 100-4000   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 100-4000
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2024-10-12
k( )
cm3s-1
Details
2.79e-12 N + NO → O + N2
T(K) = 100-4000
α = 3.75E-11
β = 0.00E+0
γ = 2.60E+1
F 0 = 0
g = 0
Type uncert: lognormal
Method: Reviews and Evaluations
Reference
Origin: Other database : UdFA
Authors:
Volume,Page:
Year:
DOI: -
Download citation:
 
Bergeat, A. et al (2009)    T(K) = 48-211   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 48-211
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2009-09-29
k( )
cm3s-1
Details
2.63e-12 N + NO → O + N2
T(K) = 48-211
α = 3.20E-11
β = 0.00E+0
γ = 2.50E+1
F 0 = 0
g = 0
Type uncert: lognormal
Method: Measurements
Description: CRESU N produced by microwave discharge and probed by VUV fluorescence
Reference
Origin: Bibliography
Authors: Bergeat, A. et al
Volume,Page: 11, 8149
Year: 2009
DOI: DOI
Download citation: Bibtex RIS
 
Baulch, D. L. et al (2005)    T(K) = 210-3700   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 210-3700
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2012-08-02
k( )
cm3s-1
Details
3.50e-11 N + NO → O + N2
T(K) = 210-3700
α = 3.50E-11
β = 0.00E+0
γ = 0.00E+0
F 0 = 1.26
g = 0
Type uncert: lognormal
Method: Reviews and Evaluations
Description: Evaluation of literature data up to 1996.
Reference
Origin: Bibliography
Authors: Baulch, D. L. et al
Volume,Page: 34, 757-1397
Year: 2005
DOI: DOI
Download citation: Bibtex RIS
 
Other database : OSU    T(K) = 10-280   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 10-280
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2009-03-27
k( )
cm3s-1
Details
2.31e-10 N + NO → O + N2
T(K) = 10-280
α = 3.00E-11
β = -6.00E-1
γ = 0.00E+0
F 0 = 2
g = 0
Type uncert: lognormal
Method: Calculations
Reference
Origin: Other database : OSU
Authors:
Volume,Page:
Year:
DOI: -
Download citation:
 
Duff, J. W. et al (1996)    T(K) = 100-1000   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 100-1000
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2024-10-12
k( )
cm3s-1
Details
2.85e-12 N + NO → O + N2
T(K) = 100-1000
α = 3.40E-11
β = 0.00E+0
γ = 2.48E+1
F 0 = 0
g = 0
Type uncert: lognormal
Method: Calculations
Description: Quasiclassical trajectory calculations on the 3A” surface of Walch, S. P.; Jaffe, R. L. The Journal of Chemical Physics 1987, 86, 6946-6956, which presents a small energy barrier (in the uncertainty).
Reference
Origin: Bibliography
Authors: Duff, J. W. et al
Volume,Page: 23, 2777-2780
Year: 1996
DOI: -
Download citation: Bibtex RIS
 
Sander, S. P. et al (2006)    T(K) = 298-298   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 298-298
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2024-10-12
k( )
cm3s-1
Details
4.63e-7 N + NO → O + N2
T(K) = 298-298
α = 2.10E-11
β = 0.00E+0
γ = -1.00E+2
F 0 = 2
g = 0
Type uncert: lognormal
Method: Calculations
Reference
Origin: Bibliography
Authors: Sander, S. P. et al
Volume,Page: xx
Year: 2006
DOI: -
Download citation: Bibtex RIS
 
Sander, S.P. et al (2011)    T(K) = 200-500   
Show/Hide those values
Channels
N + NO → O + N2
T(K): 200-500
Formula: Modified Arrhenius equation
Δ rH0 = -317.161
Δ rH298 = -314.776
2012-08-01
k( )
cm3s-1
Details
4.63e-7 N + NO → O + N2
T(K) = 200-500
α = 2.10E-11
β = 0.00E+0
γ = -1.00E+2
F 0 = 1.3
g = 100
Type uncert: lognormal
Method: Reviews and Evaluations
Reference
Origin: Bibliography
Authors: Sander, S.P. et al
Volume,Page: 10-6
Year: 2011
DOI: -
Download citation: Bibtex RIS