78
H.H. Ingelsten et al. / Journal of Catalysis 232 (2005) 68–79
mass transfer limitations and Albemarle Catalysts BV for
providing the zeolites. The KK foundation is kindly ac-
knowledged for financial support via the materials research
school (MARCHAL). This work was performed at the Com-
petence Centre for Catalysis, which is hosted by Chalmers
University of Technology and financially supported by the
Swedish Energy Agency and the member companies: AB
Volvo, Johnson Matthey-CSD, Saab Automobile Powertrain
AB, Perstorp AB, AVL-MTC AB, Albemarle Catalysts and
the Swedish Space Corporation.
Table A.1
◦
The values used for estimation of the Weisz-modulus at 450
C
r
(mol/(s kgcat))
Φ
obs
HZSM-5 40
NO
−
−
−
−
4
4
4
4
4.0 × 10
6.1 × 10
2.1 × 10
3.2 × 10
0.43
0.52
0.77
0.95
2
cat.part.
NO
2 zeolite.part.
C H
3
8 cat.part.
C H
3
8 zeolite.part.
HZSM-5 234
NO
−
−
−
−
4
4
4
4
1.7 × 10
2.6 × 10
1.2 × 10
1.8 × 10
0.18
0.23
0.44
0.54
2
2
cat.part.
NO
zeolite.part.
8 cat.part.
C H
3
C H
3
8 zeolite.part.
Appendix A. Influence of Internal diffusion limitations:
Weisz–Prater method
HZSM-5 569
NO2 cat.part.
NO
−
−
−
−
4
4
5
5
1.4 × 10
2.1 × 10
3.5 × 10
5.4 × 10
0.15
0.18
0.13
0.16
2
zeolite.part.
C H
3
8 cat.part.
The influence of mass transfer limitations in a porous cat-
alyst can be estimated by calculation of the Weiszs–modulus
C H
3
8 zeolite.part.
2
rvr
p
References
Φ =
,
(A.1)
Deffcas
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.
[
Deffcr
[
[
[
[
[
However, for the present case the catalyst particle consists
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the small zeolite particles must also be taken into account.
The effective diffusivity for the catalyst particle is estimated
−
5
as Deff,cat.part. = εpDbulk/3 = 0.35 × 2 × 10 /3 = 2 ×
−6
2
[
[
[
1
0
m /s, and the effective diffusivity for the zeolite par-
−11
2
(1992) L15.
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3
proximately 600 kg/m , the radius of the zeolite particle
[
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(
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4
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3 8
3
5
.1 mmol/m , respectively. The observed reaction rates and
the estimation of the Weisz modulus are presented in Ta-
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For all samples the calculated values of the Weiszs mod-
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[
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[
[
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