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多通道多位井速率常数的计算Rate Constants for Multi-Channel, Multi-Well Reactions
张绍文
北京理工大学
化学反应速率理论
碰撞理论(经典碰撞理论,轨线法,量子散射理论)
过渡状态理论(传统过渡状态理论,变分过渡状态理论)
过渡状态理论的基本假设
玻恩 -奥本海默近似 反应物微观状态保持玻尔兹曼分布 不返回假定 运动分离假定
化学反应速率常数的计算 正则系综速率常数的计算
传统过渡态理论
正则变分过渡态理论
TkvR
B BeQ
Q
h
TkTk /0)(
),(min)(
)(),( /)(
sTkTk
eQ
sQ
h
TksTk
s
TksvR
B B
考虑到量子隧道效应时
)()()( TkTTk
微正则系综速率常数的计算 传统过渡态理论
)(
)()(
Eh
ENEk
QeETEf
dETEfEkTk
TkE B /)(),(
),()()(
/
0
微正则变分过渡态理论
)(
)},({min)(Eh
SENEk s
隧道穿透系数的计算
BWK近似
2
1
2/1))((22
)(
x
xdxExV
m
eE
dEe
dEeET
v
TkE
TkE
B
B
0
/0
/)()(
Master Equation Method
Why Use Master Equation
• Calculate pressure dependence of rate constants• Calculate branching ratios of multi-channel
reactions• High accuracy
Single Well Multi-channel Case
B + C
D + E
F + G
A
• Methodology
A B + C
E
E0
Eik(Ei)
Ej
Rij Rji
A
B+C
ni
nj
0
)(][][
jE
iijijijiji nEkdEnRnRM
dtdn
• ni is the population of reactant molecules at energy Ei.
• [M] is the concentration of bath gas.
• Rij is the rate of collision-induced excitation from Ej to Ei of the reactant molecule on collision with a bath gas molecule (Energy transfer coefficient).
• k(Ei) is the microcanonical rate constant of the reaction at energy Ei
1. Gilbert, R. G.; Smith, S. C. Theory of Unimolecular and Recombination Reactions; Blackwell: London, 1990.
2. Klippenstein, S. J., Harding, L. B. J. Phys. Chem. 1999, 103, 9388.
3. Diau, E. W. G, Lin M. C. J. Phys. Chem. 1995, 99, 6589.
4. Robertson, S. H., Pilling, M. J., Baulch, D. L., Green, N. J. B. J. Phys. Chem. 1995, 99, 13452.
j
iiijijiji nknRnREMtn )(][
dd
j
iiijijiji nknPnPEZ
tn )(
dd
Z: collision number per unit time, collision frequency, (time-1)
Pi(E,E’): probability of energy transferred per collision, (energy-1)
ij
jiiiiijij PEZkJjiEPZJ
dt
;,
d Jnn
gJg unik kuni is pressure dependent thermal rate constants
gBg unik
1SJSB jiBfB ijiii ,0;/1
Energy Transfer Rate Coefficient
Pij=c(Ej)exp[-(Ej-Ei)/], Ei < Ej
Exponential down model
Pji f(Ei) = Pij f(Ej)
f(Ei) = [(Ei) exp(- Ei/kBT)]/Q
c(E) is normalization coefficient; is energy transfer constant; f(E) is distribution function; (E) is density of state; Q is partition function.
E
Ei
Ej
Rij Rji
1d),(0
iji EEEP
Microcanonical Rate Constant
)(
)},({min)(Eh
SENEk
R
GTSs
NGTS(E,S) is the sum of states of the Generalized Transition State (GTS).
R(E) is the density of states of the reactant.
1. Garrett, B. C.; Truhlar, D. G.; Grev, R. S.; Magnuson, A. W. J. Phys. Chem. 1980, 84, 1370.2. Hase, W. L. Acc. Chem. Res. 1998, 31, 659.3. Forst, W. Theory of Unimolecular Reactions; Academic: London, 1973. 4. Baer, T.; Hase, W. L. Unimolecular Reaction Dynamics. Theory and Experiment; Oxford: New York, 1996.5. Gilbert, R. G.; Smith, S. C. Theory of Unimolecular and Recombination Reactions; Blackwell: London,
1990.
Rate Constants for Multi-channel Reaction
B + C
D + E
F + G
A
j
iiijijiji nknRnREMtn )(][
dd
i
iij
ijijiji knnRnREMtn )(][
dd
Sum over channels
Rate Constants for Multi-Well Multi-channel Reaction
),...,()()()()()()(
)()()()()(d)(),(d
d0
'''
MIiEnEknnEfEkKEnEk
EnEkEnEkEZnEEnEEPZt
En
ipimRidiRiidi
M
ijjij
M
ijijiiE ii
i
i
1. J. A. Miller, S. J. Klippenstein, S. H. Robertson, J. Phys. Chem. A 2000, 104, 7525-7536
2. S. J. Klippenstein, J. A. Miller, J. Phys. Chem. A 2002, 106, 9267-9277
Z: collision number per unit time, collision frequency, (time-1)
Pi(E,E’): probability of energy transferred per collision, (energy-1)
Pi(E’,E) fi(E) = Pi(E,E’) fi(E’)
kij(E)j(E)=kji(E)i(E)
M
IiE idiRimR
M
IiE idi
R
ii
dEEfEkKnndEEnEkt
n00
)()()()(d
d
RmB nnn
wt
wG
d
d
N
jjj
t wggetw j
0
)0()(
Solution to the Master Equation
• Finding the eigenvalue and eigenvectors ?
• Solving the stiff ordinary differential equations ?
0.001
0.01
0.1
1
0.1 1 10 100 1000 10000
Pressure (Torr)
p
Branching fraction of product (stiff ODE results)
C2H5+O2=C2H4+HO2 的产物产率
实验 理论
Master Equation Study of HMX decomposition
H
O
H
N
H
O
N
H
OO
N
NN
N
H
O
H
N
O
HH
NO
O
H H
H HN
N
O O
O O
N N
H H
N N
O O
N
H H
H
H
H
H
H
O
H
N
N
N
N
O
O
N
N
H
N
H
O
O
O
O
N
O
O
O
N+I
II
P
0
10
20
30
40
50
Reaction Coordinate
E (
kcal
/mol
)
NO2 Fission (44.17 kcal/mol)
HONO Elimination (47.29 kcal/mol)
Potential energy profile of the HONO elimination and NO2 fission chnnels
-6
-4
-2
0
2
4
6
8
10
-3 -2 -1 0 1 2 3 4
log{P/Torr}
log{k(T,P)/s
-1}
500 K800 K1000 K1500 K
-2
0
2
4
6
8
10
-3 -2 -1 0 1 2 3 4
log{P/Torr}
log{k(T,P)/s
-1}
500 K800 K1000 K1500 K
Pressure dependent rate constants
a b
NO2 fission HONO elimination
0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
-3 -2 -1 0 1 2 3 4
log{P/Torr}
log{kNO2 (T)/k
HONO (T)} 500 K
800 K1000 K1500 K
Branching ratios vs pressure
0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
400 800 1200 1600
T/K
log{k
NO2(T)/k
HONO(T)}
0.005 Torr0.01 Torr0.05 Torr1 Torr10 Torr1000 TorrHigh pressure lim it
Branching ratios vs temperature