Print Ktpu 2
Print Ktpu 2
2 4
ANALYZING KINETIC DATA ANALYZING KINETIC DATA
5 7
Irreversible
không – 2ndbậc
thuận nghịch
2order
loại 2reaction
phân tử
or when the data are so scattered that we cannot reliably find the
Overall Order of
derivatives needed in the differential method. The integral method Irreversible Reactions from
the Half-Life
can only test this or that particular mechanism or rate form. Integral methods
CONSTANT-VOLUME
BATCH REACTOR
Irreversible Reactions in
Parallel
Differential methods Differential methods
6 8
PART A: CONSTANT-VOLUME BATCH REACTOR
p N N − a.x N a N − N
C = = = A0 = A0 −
RT V V V Δn V
❖ V = const or
1 dN i 1 d(C i V) 1 C i dV + V dC i dC i p = C RT = pA0 − (P − P ) (2.3)
ri = = = = (2.1)
V dt V dt V dt dt r
for R p = C RT = pR0 + (P − P ) (2.4)
• For ideal gases, where C = p / R T Δn
1 dpi where P0: initial total pressure of the system
ri = (2.2)
RT dt P: total pressure at time t
pA0: initial partial pressure of A
pR0: initial partial pressure of R
If the precise stoichiometry is not known, or if more than one stoichiometric equation is
needed to represent the reaction, then the "total pressure" procedure cannot be used
11
General Procedure
aA+ bB +.. = rR + sS +.. 1) Assume the rate equation
dC A dC A
At t=0 NA0 NB0 +.. = NR0 + NS0 +.. Ntr − rA = − = kf(C) − = kdt
dt f(C A )
At t NA= NA0 -ax NB= NB0 -bx NR =NR0 + rx NS =NS0 + sx, Ntr CA t
dC A
2) Integrate − = F (C A ) = k dt = kt
Initially the total number of moles C A0
f(C A ) 0
N0= NA0+ NB0+ …+NR0+ NS0+ NA0+.. Ntr
At time t it is
3) Calculate F(CA) by experimental data
N = N0 + x (r+ s+ … – a –b – …) = N0+ x n
4) Plot F(CA) vs. t
where n = r+ s+ … – a –b – …
𝑁−𝑁
x= 5) If the fit is unsatisfactory, another rate equation is
∆𝑛
10 guessed and tested
không thuận nghịch
Irreversible- bậc
1st order
1, loại 1 phânA→P
tử A→C
reaction
(1) Irreversible Unimolecular-Type First-Order Reactions A P
Irreversible
không – 2ndbậc
thuận nghịch
2order
loại 2reaction
phân tử
Zero-Order
baäc Reactions
0
A PRODUCTS dC A
− = k CA
nthbậOrder
cn dt
Overall Order of
Irreversible Reactions from
the Half-Life CA
Integral methods t
dC A
CONSTANT-VOLUME
BATCH REACTOR − = k dt
Differential methods
Irreversible Reactions in
Parallel
C A0
C A 0
Interpretation of kinetic
data Irreversible Reactions in
Series
A→R→S
Integral methods
CA
VARYING-VOLUME
BATCH REACTOR
First-Order Reversible
− ln = kt
(ε0) Reactions :
A ↔ R
C A0
Differential methods
13 15
First-Order dX
Irreversible
Reversible Reactions ⇒ = k dt ⇒ − ( − 𝐀) =
Reactions in Series 1 − X
A R
A→R→S
14 16
(1) Irreversible Unimolecular-Type First-Order Reactions (2) Irreversible Bimolecular-Type Second-Order
A P Reactions A + B→ Products
Caution. - dCA/dt = kCA 0,6.. CB0,4 are first order but are not enable to this kind
of analysis; hence, not all first- order reactions can be treated as shown above. dC dC
− = − = k C .C (2.12)
dt dt
the amounts of A and B that have reacted at any time t are equal and given by CAoXA
CAo X = CBo X
dX
CA𝑜 = k ( CA𝑜 − CA𝑜 . X )(CB𝑜 − CA𝑜 . X )
dt
( CA = CA𝑜 − CA𝑜 . X
CB = CB𝑜 − CB𝑜 . X = CB𝑜 − CA𝑜 . X )
𝐂 𝒐
letting =
𝐂 𝒐
17 20
dt 𝒐
− 𝐁 − 𝐀 𝐂𝐁 . 𝐂𝐁
= = =
− 𝐀 ( − 𝐀) 𝐂 𝒐 𝐀 𝐀
= ( − ) = (𝐂 𝒐 −𝐂 𝒐) ≠
𝐂 𝒐
=
𝐂 𝒐
−𝑑𝐶
= 𝑘𝐶 𝐶 = 𝑘𝐶 1 − 𝑋 𝑀 − 2𝑋 ; 𝑴 ≠ 𝟐
𝑑𝑡
C 𝐶 𝑀 − 2𝑋
ln = ln = 𝐶 (𝑀 − 2)𝑘𝑡; 𝑴≠𝟐
CBo 𝐶 𝑀(1 − 𝑋 )
Caution 1: Equal initial concentrations of A and B (M=1) (2) Irreversible Bimolecular-Type Second-Order
or: Reactions A + B→ Products
a) 2A → products EXAMPLE A.1.2 (3.22)
dC
− = kC = kC A𝑜 (1 − X ) (2.14𝑎) For the reaction A →R, second-order
dt
kinetics and CA0 = 1mol/liter, we get 50%
− = . = kt (2.14𝑏) conversion after 1 hour in a batch reactor.
Ao Ao 1 X
What will be the conversion and
concentration of A after 1 hour if CA0 = 10
2.14b mol/liter?
2.14b
23 25
(3) Empirical Rate Equations of nth Order (4) Zero-Order Reactions
dC The rate of reaction is independent of the concentration of materials
− = kC
dt dC
− = k
dt
1 n = ( n − 1)kt, n ≠ 1
C 1 n − CA (2.21)
𝑜 − = CAo X = , t<CA0/k (2.24)
𝒐 𝐀
CA=0, t ≥ CA0/k
1 n
CA0 1 − X n − 1 = (n − 1)kt (2.22)
27 31
(3) Empirical Rate Equations of nth Order (5) Overall Order of Irreversible Reactions from the Half-Life
t1/2
these kinetics. −
dC
= k C
dt
𝟐
⇒ = (𝟐. 𝟐𝟔) (n ≠ 1 )
𝐤 ( )
CR − CR 0 k1
= Slope k1/k2
C S − C S0 k2
Plot CR vs Cs → k1/k2
35
dC
+r = + = k C
dt
dC
+r = + = k C
dt
A → R → S , k1 & k2 e k − e k
C = k CAo
k − k
No R or S present, initial concentration of A: CAo
C
𝑑𝐶
=0 k2
ln
− ln = k t 𝑑𝑡
dC A C
= − k1 C A
dt C =C e k 1 k1
t max = =
dC
+ k C = k CA0 e k
k log tb k 2 − k1
dC R dt
→ The maximum concentration
= + k1 C A − k 2 C R dy/dx+Py=Q
dt of R:
k 2 / ( k 2 − k1 )
e k − e k
C R, max k1
dC S
= + k 2 CR
C = k CAo
k − k
= Typical concentration-time curves
dt C A0 k2
for consecutive first-order reactions.
37 2.42 39
k ⟩⟩ k C = CAo 1 − e
→ the rate is determined by k1, or the first step of the two-
step reaction.
k ⟩⟩ k C = CAo 1 − e A → R → S , k1 , k2
38 40
(8) First-Order Reversible Reactions: A ↔ R
k1
k (8) First-Order Reversible Reaction
KC = K = equilibrium constant
2
C Re C Ro + C Ao X A e k
KC = = = 1
C Ae C Ao − C Ao X A e k2
41 43
Irreversible
không – 2ndbậc
thuận nghịch
2order
loại 2reaction
phân tử
dX A
= (k 1 + k 2 )(X Ae − X A ) Zero-Order
baäc Reactions
0
dt
nthbậOrder
cn
X C − CA e 1 Overall Order of
= − ln A = k 1 1 + t = (k 1 + k 2 )t
Irreversible Reactions from
− ln1 − A C −C K Integral methods the Half-Life
X Ae A0 Ae C CONSTANT-VOLUME
BATCH REACTOR
the irreversible reaction is simply the special case of Integral methods A→R→S
VARYING-VOLUME
42 45
A.2. Differential Method of Analysis of Data CONSTANT-VOLUME
BATCH REACTOR
Procedure:
p N N − a.x N a N − N
1. Plot the CA vs. t data, and then by eye carefully draw a C = = = A0 = A0 −
smooth curve to represent the data. This curve most likely will RT V V V Δn V
not pass through all the experimental points. or
2. Determine the slope of this curve at suitably selected p = C RT = pA0 − (P − P ) (2.3)
concentration values. These slopes dCA/dt = rA are the rates of
reaction at these compositions. r
for R p = C RT = pR0 + (P − P ) (2.4)
3. Search for a rate expression to represent this rAvs. CAdata Δn
where P0: initial total pressure of the system
P: total pressure at time t
pA0: initial partial pressure of A
pR0: initial partial pressure of R
If the precise stoichiometry is not known, or if more than one stoichiometric equation is
needed to represent the reaction, then the "total pressure" procedure cannot be used
46 48
Zero-Order
baäc Reactions
0 Example A.1.9
nthbậOrder
cn
Consider the following gas phase reactions,
express the relationship between the total
Overall Order of
Irreversible Reactions from pressure of the system and partial pressure of the
the Half-Life
Integral methods
reacting materials:
CONSTANT-VOLUME
BATCH REACTOR
Irreversible Reactions in a. N2O4→2 NO2
Parallel
Differential methods
b. N2O →N2 + ½ O2
Interpretation of kinetic
data Irreversible Reactions in
Series
c. N2O5 →N2O4 + ½ O2 with 60 mole % N2O5 and
VARYING-VOLUME
Integral methods A→R→S
40 mole % inerts initially.
BATCH REACTOR
First-Order Reversible
(ε0) Reactions :
Differential methods A ↔ R
47 49
không thuận nghịch bậc
1, loại 1 phân tử A→C
Zero-Order Reactions
CONSTANT-VOLUME
BATCH REACTOR PART B: VARYING-VOLUME BATCH REACTOR
A reaction is of zero order when the rate of reaction is = 𝟏 + 𝜺𝐀 𝐀 → Volume of reaction system
𝟎
independent of the concentration of the reactant. 𝐕𝐗𝐀 − 𝐗𝐀
dC 𝜺𝐀 = eA is the fractional change in volume of the
−
dt
= k 𝐕𝐗 𝐀 system between no conversion and complete
conversion of reactant A.
𝒐 − 𝐀 = CAo X = , t<CA0/k (2.24)
CA=0, t ≥ CA0/k
Example A.1.11
EX: Considering isothermal gas phase reaction A 4R
The composition of gas A →2.7 R is zero order reaction, occurs in a constant volume by starting with pure A reactant:
reactor (following with the results in the table). The initial mixture contains 80 mole % 4 − 1
A and 20 mole % inerts. 𝜀 = =3
a. If the initial total pressure is 10 at, with pure A, find the toal pressure after 1 h. 1
b. If the initial partial pressure of A is 1 at, of inert is 9 at, find the total pressure after
1h. with 50% inerts present at the start:
t (h) 0 1
5 − 2
Total pressure (at) 1 1.5 𝜀 = = 1.5
2
53 55
PART B: VARYING-VOLUME BATCH REACTOR PART B: VARYING-VOLUME BATCH REACTOR
VX A = 1 − VX A = 0 fractional change in
eA = volume of the system
VX A = 0
56 58
C =
N N
= A0
1 − X
𝐶𝐴 = CAo
1 − X 1- Zero order: the rate of reaction is independent of
1 + 𝜀 X
V V 1 + 𝜀 X
the concentration of the reactant.
1 dN CA0 dX
−r = − = =𝑘
V dt 1 + 𝜀 X dt
𝐶 ∫ = ln( 1 + 𝜀 𝑋 ) = ln = 𝑘𝑡 (2.63)
𝑽 − 𝑽𝒐 ∆𝑽
1 dN 1 NAo d 1 − X = 𝟎 𝟏 + 𝜺𝑨 𝑨 ⇒ 𝑨 = =
𝑽 𝒐 𝜺𝑨 𝑽𝒐 𝜺𝑨
−r = − = −
V dt V 1 + 𝜀 X dt
(2.63)
CAo dX
=
1 + 𝜀 X dt (2.63)
57 59
PART B: VARYING-VOLUME BATCH REACTOR PART B: VARYING-VOLUME BATCH REACTOR
XA (1 + e A X A )n −1
o (1 − X A )n
dX A = C nA−1 k t
o
61 64
PART C: TEMPERATURE AND REACTION RATE PART C: TEMPERATURE AND REACTION RATE
E 1
lnk = ln A − Example C.2
Arrheùnius law RT
-E/R
ln k
The activation energy of a chemical reaction
k = k0 e- E / RT
is 17982 cal/mol in the absence of a
whereas:
1/T
catalyst, and 11980 cal/mol with a catalyst.
k0: frequency factor By how many times will the rate of the
E : activation energy, J/mol reaction will grow in the presence of a
R: 8.27 J/mol.K catalyst, if a reaction proceeds at 25°C?
T: K
65 68
Example C.1
A common rule of temperature is that the rate
of the reaction doubles for each 10°C rise in
temperature. What activation energy would
this suggest at a temperature of 25 °C?
66 71
72