coking characteristics of dry methane reforming by dbd ... · by dbd-catalyst hybrid reaction with...
TRANSCRIPT
I. INTRODUCTION
CH4 is the main component of natural gas and biogas.
However, it has a poor energy density because it is gas in
the standard condition. Table I shows the energy density
of various energy sources. A carbon-containing liquid
fuel has higher volumetric energy density than other
forms of energy. Therefore CH4 should be converted into
liquid fuel via syngas (H2 and CO).
In commercialized CH4 reforming, initial CH4 is
partially combusted in order to obtain high temperature
thermal energy (> 800°C). Non-thermal plasma has low gas temperature and high electron temperature, then gas
molecules can be activated at low temperature by
colliding with high temperature electrons. It leads to
reactions without a limitation of thermal equilibrium.
Because of that, to lower the reaction temperature, many
studies for CH4 reforming using plasma have been
investigated [3–11] ([3–5]: steam methane reforming, [6–
8]: dry methane reforming, [9–11]: methane partial
oxidation).
Commercialized syngas production from CH4 is
steam methane reforming (SMR), as in (1). However,
SMR produces CO2 by water-gas shift (WGS) reaction,
as in (2). In order to reduce CO2 emission, dry methane
reforming (DMR), as in (3), is desired.
CH4 + H2O → CO + 3H2 (1)
CO + H2O → CO2 + H2 (2)
CH4 + CO2 → 2CO + 2H2 (3)
However, in DMR, solid carbon deposition (coking) is
inevitable as shown in Fig. 1 [12]. It describes that
carbon limit is clarified by O/C and H/C ratios of raw
material. Curves A and B represent the carbon limit
criteria, showing whisker (left side of B) and graphite
(left side of A) formation limit. Deposited carbon
deactivates and eventually destroys the catalysts in
several ways: surrounding and blocking access to the
active phase surface, encapsulating the active metal
particles, plugging the pores, accumulating as strong
Coking Characteristics of Dry Methane Reforming
by DBD-catalyst Hybrid Reaction with Cyclic Operation
S. Kameshima, K. Tamura, Y. Ishibashi, and T. Nozaki
Department of Mechanical Sciences and Engineering, Tokyo Institute of Technology, Japan
Abstract—Dry methane reforming is promising technology to reduce CO2 emission. However, high temperature
(> 800°C) is favor for the dry methane reforming by thermal reaction, and catalysts are deactivated and destroyed by
coking, which is the major issue in the dry methane reforming. In this work, we succeeded the long time operation at low
temperature by using DBD-catalyst hybrid reaction combined with cyclic operation, which conducted reforming and de-
coking reactions alternatively by pulsed methane supply. Plasma heating promoted reactions, and de-coking time was
reduced by 35% from thermal reaction. CO formation in reforming was dominated by the reactions of CO2-CHx and CO2-
H. In contrast, Boudouard reaction (C + CO2 → 2CO) eliminating solid carbon on catalysts has small contribution in
reforming. This is caused by the difference of the reaction rates.
Keywords—Dry methane reforming, methane, carbon dioxide, syngas, hybrid reaction, plasma
TABLE I
COMPARISON OF ENERGY DENSITY
Energy density
[kWh/L] Ref.
Hydrogen (207 bar) 0.50 [1]
Natural gas (207 bar) 2.8 [1]
Methanol 4.4 [1]
Li-ion battery 0.22-0.4 [2]
Corresponding author: Tomohiro Nozaki
e-mail address: [email protected] Presented at the 3rd Korea-Japan Conference on Plasma and
Electrostatics Technologies, in November 2014
Fig. 1. Carbon limit diagram [12], A: graphite, B: whisker carbon.
(Original figure adopted from [12] was modified.)
40 International Journal of Plasma Environmental Science & Technology, Vol.9, No.1, APRIL 2015
carbon filaments leading to catalyst disintegration, and
physically blocking the reactor [13]. Therefore,
countermeasures for coking are essential. We achieved to
carry out DMR while controlling coking by conducting
solid carbon removal (de-coking) through Boudouard
reaction (4) in CO2 plasma generated cyclically by pulsed
CH4 supply [14, 15].
C + CO2 → 2CO (4)
To avoid catalyst deactivation, the deposited carbon must
be removed before it grows thick layer of carbon
filaments. In this study, we investigated both of hybrid
and thermal reaction in order to discuss the coking issue
and the contribution of non-thermal plasma.
II. METHODOLOGY
A. DBD-catalyst Hybrid Reactor
Experimental setup is shown in Fig. 2. The inner
diameter of the reactor was 20 mm, and the high voltage
electrode with 3 mm diameter was fixed in an axis of the
quartz tube. The grounded electrode length was 20 mm,
and it had a 10 mm width slit to measure the catalyst bed
temperature by infrared camera (TH5104, NEC San-ei
Instruments, Ltd.). 12wt%/Al2O3 catalysts with 3 mm
mean diameter was used for the experiments. Catalysts
were reduced for 90-min in H2/N2 = 50/450 cm3/min with
600°C prior to the experiment.
B. Cyclic Operation and Analysis
Feed gas was changed periodically by turning CH4
flow on and off with duty ratio of 25%. During cyclic
operation, CO2 was supplied continuously. Feed gas for
the reforming reaction was CH4/CO2 = 2 and 10300 h-1
GHSV (gaseous hourly space velocity, as in (5)). For the
de-coking reaction, GHSV decreased to one third
because only CO2 was supplied. Discharge power and
frequency were 71 W and 12.5 kHz, respectively.
GHSV [h−1] =60 × (𝑡𝑜𝑡𝑎𝑙 𝑓𝑙𝑜𝑤 𝑟𝑎𝑡𝑒 [cm3/min])
(𝑟𝑒𝑎𝑐𝑡𝑖𝑜𝑛 𝑣𝑜𝑙𝑢𝑚𝑒 [cm3])
(5)
Within the product gas, H2, CH4, CO, O2 and CO2
were analyzed by QMS (quadrupole mass spectrometer,
Prisma, Pfeiffer Vacuum Technology) after trapping
liquid components by cold trap (ca. -40C). Pressure was
decreased to 5 kPa because DBD was extinguished when
solid carbon, which is electrically conductive material,
was formed on the catalyst surface.
III. RESULTS
Long Time Operation
Both hybrid and thermal operations were conducted
for 56-min, 14 cycles. Feed gas was supplied with
CH4/CO2 = 2, duty ratio = 25% and cycle time = 4-min.
The result of hybrid reaction is shown in Fig. 3. It shows
that the cyclic operation made long time stable operation
possible. Fig. 4 (a) focuses on the last 3 cycles of Fig. 3.
Fig. 4 (b) is the last 3 cycles of full operation by thermal
reaction. Before the reaction, catalyst bed temperature
was elevated in N2 flow until steady state temperature
distribution was established. This temperature is defined
as initial temperature as shown in Fig. 4.
Fig. 2. DBD-catalyst hybrid reactor.
Fig. 3. Long time operation (14 cycles, 56-min) by hybrid reaction.
Kameshima et al. 41
IV. DISCUSSION
A. Plasma heating
Table II shows conversions, solid carbon selectivity
and yield defined as (6-9).
CH4 𝑐𝑜𝑛𝑣. =𝑖𝑛𝑝𝑢𝑡 𝐶𝐻4 − 𝑜𝑢𝑡𝑝𝑢𝑡 CH4
𝑖𝑛𝑝𝑢𝑡 CH4
(6)
CO2 𝑐𝑜𝑛𝑣. =𝑖𝑛𝑝𝑢𝑡 𝐶𝑂2 − 𝑜𝑢𝑡𝑝𝑢𝑡 CO2
𝑖𝑛𝑝𝑢𝑡 CO2
(7)
C(s) 𝑠𝑒𝑙. =C(s)
𝑐𝑜𝑛𝑣𝑒𝑟𝑡𝑒𝑑 C
=C(s)
𝑐𝑜𝑛𝑣𝑒𝑟𝑡𝑒𝑑 CH4 + 𝑐𝑜𝑛𝑣𝑒𝑟𝑡𝑒𝑑 CO2
(8)
C(s) 𝑦𝑖𝑒𝑙𝑑 =C(s)
𝑖𝑛𝑝𝑢𝑡 C
=C(s)
𝑖𝑛𝑝𝑢𝑡 CH4 + 𝑖𝑛𝑝𝑢𝑡 CO2
(9)
The moles of deposited carbon is same as the moles of
converted CO2 during the de-coking process because
carbon and CO2 react 1:1 molar ratio according to
Boudouard reaction (4). Deposited carbon is estimated by
(10), which is denoted by the area Ah or At in Fig. 4.
C(s) = 𝐴ℎ (𝑜𝑟 𝑡) = ∫ (𝑄𝐶𝑂2 × CO2 𝑐𝑜𝑛𝑣. )𝑑𝑡𝑑𝑒−𝑐𝑜𝑘𝑖𝑛𝑔
(10)
As shown in Fig. 4, the time for de-coking by thermal
reaction was 1.5 times long as hybrid reaction even
though the amount of deposited carbon were almost same,
as in Table II. It might be caused by the temperature
difference. Operating temperature of hybrid reaction was
higher than that of thermal reaction. However, initial
temperature of hybrid reaction was lower than that of
thermal reaction. Plasma generates not only radicals but
also heat internally. Plasma enables internal heating, so
efficient heat supply was possible and it resulted in high
conversions and short de-coking time.
B. CO formation and coking
In Fig. 4, at the moment of turning CH4 flow on and
off, the increase of CO mass spectrum intensity, as
described by arrows in Fig. 4, were different. Namely, it
Fig. 4. Last 3 cycles of cyclic operation (14 cycles, 56-min). (a): hybrid reaction, (b): thermal reaction.
TABLE II
MEAN CONVERSIONS, SOLID CARBON SLECTIVITY AND YIELD
IN REFORMING OF LAST CYCLE
CH4 conv. CO2 conv. C(s) sel. C(s) yield
Hybrid 0.60 0.77 0.17 0.11
Thermal 0.46 0.60 0.24 0.12
TABLE III
RATE CONSTANTS [17]
T [°C] k [s−1]
(CO2 – adsorbed CHx)
k [s−1]
(CO2 – C)
440 1.8 × 10−2 2.5 × 10−3
484 5.0 × 10−2 4.1 × 10−3
560 − 6.7 × 10−3
42 International Journal of Plasma Environmental Science & Technology, Vol.9, No.1, APRIL 2015
increased sharply when CH4 was supplied, but it increase
gradually when CH4 was stopped. It indicates that the CO
formation mechanism during the reforming and the de-
coking process are different.
As DMR mechanism on the nickel catalysts, following
series of reactions is widely accepted [16].
CH4 + (5 – x) * → CHx* + (4 – x) H* (11)
CO2 + H* → CO + OH* (12)
CHx* + OH* → CHxO* + H* (13)
CHxO* → CO* + x/2 H2 (14)
CO* → CO + * (15)
2H* → H2 + 2* (16)
Here, * denotes adsorbed species on active sites of
catalysts. First, CH4 is adsorbed and dissociated to CHx
and H on the catalysts (11). Subsequently, the adsorbed
species react with CO2 (12)-(15) and desorption of H2
occur (16). (12)-(15) can be summarized into (17). It is
the CO formation mechanism in the reforming process.
CO2 + CHx* → 2CO + x/2 H2 + * (17)
On the other hand, in the de-coking process, CO is
produced from solid carbon and CO2 via Boudouard
reaction (4). According to Osaki et al, the rate constant
on Ni/Al2O3 catalyst of (17) is faster than that of (4) [17],
as shown in Table III. Due to the above, CO2-CHx and
CO2-H reactions are dominant pathway for CO formation,
so CO mass spectrum intensity increased sharply when
CH4 supply was started. However, when CH4 supply was
stopped, only Boudouard reaction (4) whose rate is slow
compared with (17) was possible, so the increase of CO
mass spectrum intensity is slow.
CH4 adsorption (11) finally forms solid carbon (18).
CH4 → (CH3* → CH2* → CH* →) C* (18)
Intermediates and final product of (17), CHx and C, are
converted into CO via (17) and (4), respectively. If the
rate of CO formation was faster than that of (18), coking
didn’t occur, however, solid carbon was formed. It
suggests that the rate of coking (18) is fast.
V. CONCLUSION
In this work, long time (56-min) operation of DMR
was succeeded, and it was implied that the CO formation
rate in the reforming process was faster than in the de-
coking process. This suggests that reactions by CO2-CHx
and CO2-H are dominant in CO formation of reforming.
However, CO formation reactions, CO2-CHx, CO2-H and
CO2-C reactions, are slow compared with CH4
decomposition, then carbon is accumulated. Heat
generated by DBD could heat up the catalysts, so
reforming and de-coking reactions were promoted,
thereby CH4 and CO2 conversions increased to 0.60 from
0.46 and 0.77 from 0.60 in reforming, respectively, and
de-coking time was shortened by 35%, even when the
initial temperature was low.
REFERENCES
[1] M. Gattrell, N. Gupta, and A. Co, "Electrochemical reduction of CO2 to hydrocarbons to store renewable electrical energy and
upgrade biogas," Energy Conversion and Management, vol. 48,
pp. 1255-1265, 2007. [2] J. M. Tarascon and M. Armand, "Issues and challenges facing
rechargeable lithium batteries," Nature, vol. 414, pp. 359-367,
2001. [3] Q. Liu, H. Zheng, R.Yang, and G. Pan, "Experimental study on
chemical recuperation using hybrid dielectric barrier discharge-
catalytic methane-steam conversion," Proceedings of the
Institution of Mechanical Engineers, Part A: Journal of Power
and Energy, vol. 228, pp. 451-461, 2014.
[4] B. Pietruszka and M. Heintze, "Methane conversion at low temperature: the combined application of catalysis and non-
equilibrium plasma," Catalysis Today, vol. 90, pp. 151-158, 2004.
[5] I. Rusu and J. M. Cormier, "On a possible mechanism of the methane steam reforming in a gliding arc reactor," Chemical
Engineering Journal, vol. 91, pp. 23-31, 2003.
[6] H. J. Gallon, X. Tu, and J. C. Whitehead, "Effects of reactor packing materials on H2 production by CO2 reforming of CH4 in
a dielectric barrier discharge," Plasma Processes and Polymers,
vol. 9, pp. 90-97, 2012. [7] M. Kraus, W. Egli, K. Haffner, B. Eliasson, U. Kogelschatz, and
A. Wokaun, "Investigation of mechanistic aspects of the catalytic
CO2 reforming of methane in a dielectric-barrier discharge using optical emission spectroscopy and kinetic modeling," Physical
Chemistry Chemical Physics, vol. 4, pp. 668-675, 2002.
[8] V. Goujard, J. M. Tatibouet, and C. Batiot-Dupeyrat, "Carbon
dioxide reforming of methane using a dielectric barrier discharge
reactor: effect of helium dilution and kinetic model," Plasma
Chemistry and Plasma Processing, vol. 31, pp. 315-325, 2011. [9] B. Pietruszka, K. Anklam, and M. Heintze, "Plasma-assisted
partial oxidation of methane to synthesis gas in a dielectric
barrier discharge," Applied Catalysis A-General, vol. 261, pp. 19-24, 2004.
[10] S. Jo, D. H. Lee, and Y. H. Song, "Effect of gas temperature on
partial oxidation of methane in plasma reforming," International Journal of Hydrogen Energy, vol. 38, pp. 13643-13648, 2013.
[11] C. H. Tsai and T. H. Hsieh, "New approach for methane
conversion using an rf discharge reactor. 1. Influences of operating conditions on syngas production," Industrial &
Engineering Chemistry Research, vol. 43, pp. 4043-4047, 2004.
[12] J. R. Rostrup-Nielsen and J. Bøgild Hansen, "Steam reforming for fuel cell," in Fuel Cells: Technologies for Fuel Processing, Ed. D.
Shekhawat, J. J. Spivey and D. A. Berry, Amsterdam: Elsevier, 2011, ch. 4, pp. 49-71.
[13] A. M. Amin, E. Croiset, and W. Epling, "Review of methane
catalytic cracking for hydrogen production," International Journal of Hydrogen Energy, vol. 36, pp. 2904-2935, 2011.
[14] S. Kameshima and T. Nozaki, "Low-temperature dry methane
reforming in non-equilibrium plasma and catalyst hybrid reaction (in Japanese)," Journal of Institute of Electrostatics Japan, vol.
38, pp. 228-233, 2014.
[15] S. Kameshima, K. Tamura, S. Moore, and T. Nozaki, "Effect of reverse water-gas shift and methanation reactions on plasma-
assisted dry methane reforming (in Japanese)," in Proceedings of
2014 Annual Meeting of the Institute of Electrostatics Japan, pp. 75-76, 2014.
[16] J. Gao, Z. Hou, H. Lou, and X. Zheng, "Dry (CO2) reforming," in
Fuel Cells: Technologies for Fuel Processing, Ed. D. Shekhawat, J. J. Spivey and D. A. Berry, Amsterdam: Elsevier, 2011, ch. 7,
pp. 191-221.
[17] T. Osaki, T. Horiuchi, K. Suzuki, and T. Mori, "Kinetics, intermediates and mechanism for the CO2-reforming of methane
on supported nickel catalysts," Journal of the Chemical Society-
Faraday Transactions, vol. 92, pp. 1627-1631, 1996.
Kameshima et al. 43