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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 605
A passive DMFC with membrane for diffusion controlled methanol feed
A. Balasubramanian1, R. Vijayakumar2
1Assistant Professor, Department of Petroleum Engineering, AMET University, Chennai – 603112, India
2Chemical Testing and Analytical Laboratory, Guindy, Chennai – 600 032, India
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract - Transport of methanol to the anode of a passive
Direct Methanol Fuel Cell (DMFC) forvaryingconcentrationof
methanol was studied using Nafion membranes of varying
thickness namely, 50, 125, 175m. Themaximumpowerdensity
was achieved with 1M aqueous methanol in the case of Nafion
112 as passive methanol transport layer (PMTL). Higher
power density was achieved with 4M aqueous methanol while
the power density decreased for concentrations higher than
4M in the case of Nafion 115 and Nafion 117. Maximumpower
density of 21 mW cm-2 was obtained with Nafion 115
membrane as PMTL for 4M aqueous methanol at ambient
conditions.
Key Words: Passive Direct Methanol Fuel Cell; Transport;
Methanol; Membranes; Power density.
1. INTRODUCTION
Direct methanol fuel cells (DMFCs) have been an important
area of research for application in portable electronic
devices, such as notebook computers, personal digital
assistants (PDAs), music systems and cellular telephones
due to their advantages in terms of high energy density,
simplicity and fast recharging [1-3]. However, in order
to be commercially feasible, it is necessary to eliminate
power losses from auxiliaries such as fuel and reactantfeed
pumps, methanol and liquid level sensors, which are used in
the active DMFCs. Passive DMFCs without such auxiliaries,
have much simpler structures and are being investigated[4-
6].
Operating parameters and design of the passive DMFCs are
crucial to enhance their performance. The operating
parameters such as temperature, methanol flow rate and its
concentration, and designaspectslikepassivemethanol feed
system, CO2 removal from anode are mainly limiting the cell
performance. The optimal methanol concentration was
reported to be 4.0 M for passive DMFCs [7, 8]. Yang et al. [9]
reported that much higher exposureratiooftheparallel flow
field on the anode and perforated flow field on the cathode
increased the delivery of fuel and oxygen, respectively
resulting in enhanced performance. In passive DMFCs [10],
higher temperature at cathode improves natural convection
due to temperature difference between the MEA and the
atmospheric air leading to enhanced performance.
Presently, one of the most challenging problems for the
passive DMFCs is supply of methanol at a desired flow rate
and concentration from the reservoir tank to the anode.
However, high and low methanol concentration lead to
methanol crossover with resultant mixed potential on the
cathode and low energy density, respectively [10]. Hence,
some researchers [11-16] have made improvements in the
fuel delivery system to increase the methanol feed
concentration. Abdel kareem et al. [11-13] reported that
while employing a porous carbon plate because of the
increased mass transfer resistance higher concentration of
methanol could be used. Kim et al. [14, 15] employed
hydrogels in methanol fuel cartridges to control methanol
diffusion rate from the fuel reservoir to the anode. Yangand
Liang [16] reported on a DMFC system with passive fuel
delivery based on liquid surface tension. In the present
study, we report on the use of Nafion membrane of varying
thickness as passive methanol transport layer (PMTL) for
supply of methanol; in a diffusion-controlled mode to the
anode. To the best of our knowledge, thiskindofapproachof
passive delivery of methanol to the anode has not been
reported.
2. EXPERIMENTAL
Exploded view of passive DMFCs as shown in Fig. 1(A), was
designed, fabricatedand tested in this study. The membrane
electrode assembly (MEA) procured from M/s Johnson
Matthey used in this study had 4 mg cm-2 loading of carbon-
supported 1:1 Pt/Ru catalyst on the anode and 2 mg cm-2
loading of carbon-supportedPtonthecathode.ThisMEAwas
sandwiched between anode and cathode graphite flow field
plate, which was then clamped between two transparent
acrylic fixture plates. Anode and cathode flow field plate
machined into parallel windows and perforated holes,
respectively. A step of 0.5 mm width and 0.5 mm depth was
machined along the circumference of the parallel windows
forremoval of CO2as shown in Fig. 1(B).Areservoirof5.0mL
capacity was built in the anode fixture. 1M methanolsolution
from the built-in reservoirwassuppliedtotheanodereaction
zone through PMTL (Nafion 117 membrane) which was
assembled between methanol reservoir tank and the anode
flow field plate. Atmospheric air was supplied as an oxidant
to the cathode reaction zone by natural convection. Bitrode
T2000 electricalload interfacedtoacomputerwasemployed
to record the voltage - current curves. The polarization
curves were obtained in potentio static mode and discharge
current was obtained at a constant voltage of 0.4V. At three
current densities like 25, 50 and 75 mA cm-2 the
concentration of CO2 gas (in ppm) was measured by using
CO2 gas sensor (Vaisala CO2 sensor M170) as shown in Fig. 1
1(B). Similarlyelectrochemicalexperimentswerecarriedout
with Nafion 115 and 112 membranes as PMTL for varying
methanol concentration (1M, 2M, 3M, 4M and 5M).
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 606
Fig-1: (A) Schematic of exploded view of the passive
DMFCs cell fixture. (B) Provision for CO2 removal in a
passive DMFC
3. RESULTS AND DISCUSSION
The amount of methanol delivery by passive feeding
(diffusion) to reaction layer from reservoir is a function of
methanol concentration and PMTL thickness that
determines the cell performance. In Chart 2, the influence of
the PMTL such as Nafion 112; Chart 2(A), Nafion 115; Chart
2(B), and Nafion 117; Chart 2(C) with varying methanol
concentration (1M, 2M, 3M, 4M and 5M) on theperformance
of passive DMFCs are given. In Chart 2 (A), it is clearly seen
that higher performances at 1 and 2M while lower
performances at 3, 4, and 5M methanol are obtained. With
increase in methanol concentration increased methanol
crossover resulted in decreased performance. Chart 2(C)
shows that on replacement of PMTL i.e. Nafion 112 with
Nafion 117, comparatively low performance at lower
concentrations (1M and 2M) and enhanced performance at
higher methanol concentrations (3M and 4M) are obtained,
which is attributed to the decrease in methanol transport
flux (MTF) due to increase in PMTL thickness from 50 to
175 m. Chart 2(B) shows the results obtained on
replacement of PMTL i.e. Nafion 112 with 115. The
polarization curves obtained for methanol concentrations
1M, 2M and 3M follow similar trend. A peak power density
of 21 mW/cm-2 is obtained with 4.0 M methanol. However,
in all cases with 5 M methanol, the OCVdecreased,indicating
that significant methanol crossover from anode to cathode
causes decrease in cell performance. The maximum power
density is obtained for optimal passive methanol feeding by
diffusion with PMTL using Nafion 115 membrane and 4M
methanol. In passive DMFC single cell studies, the methanol
crossover and methanol transportfluxareobtainedfromthe
following equations.
Initial volume in the reservoir
Volume methanol crossed over Final volume in the reservoir
Volume reacted
 
 
  
 
 
(1)
Volume of methanol crossed over
Volume of methanol used for oxidation
Methanol Transport Flux
Area of PMTL Time
 
 
 
 
 
 
(2)
Chart. 1: Effect of passive methanol transport layer (A)
Nafion 112, (B) Nafion 115 and (C) Nafion 117 membrane
for varying methanol concentrations on performance of
passive DMFCs.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 607
Initial and final volume of methanol in the reservoir is
noted for each test. Volume of methanol reacted is
equivalent to faradaic oxidation of methanol. At constant
current density of 40 mA cm-2, the methanol crossover
current density and MTF are calculated using the above
equations, for various methanol concentrations and for
different PMTL and the data are shown in Chart 2. Increase
in the thickness of the PMTL from 50 to 175 m leads to
decrease in MTF thus limiting the mass transport to the
anode and consequently, methanol crossover in passive
DMFCs.
Chart. 2: Methanol crossover current density (solid lines)
and methanol transport flux (dotted lines) with respect to
varying methanol concentrations at 40 mA cm-2.
The concentrations of CO2 at 25, 50 and 75 mA cm-2 are 420,
500 and 590 ppm, respectively. It is interesting to note that
the measured concentration in ppm corresponds to the
faradaic oxidation of methanol. The discharge current
behavior of the cell is also tested at varying methanol
concentrations at a constant voltage of 0.4V with different
PMTLs as shown in Chart 3. The discharge current density
obtained for 5M concentration is less than that for 4M
concentration reiterating the fact that MTF is optimal at 4M
concentration. A maximum load current density of 33 mA
cm-2 obtained with PMTL of Nafion 115 membrane at 4.0 M
methanol can be attributed to the optimized PMTL and
methanol concentration.
Chart. 3: Discharge current density at a constant voltage
(0.4V) with different passive methanol transport layers:
(A) Nafion 112, (B) Nafion 115 and (C) Nafion 117 for
varying methanol concentrations.
In order to evaluate whether the passive DMFCs suffer from
the oxygen mass transport limitation on the cathode, the
limiting current density was measured with forced air on
the cathode of a passive DMFC, also called as a semi-passive
DMFC. Chart 4 shows the performance curve of passive and
semi-passive DMFCs with optimized PMTL of Nafion 115
membrane and 4M methanol solution. In the performance
curves, a difference in limiting current density of 15 mA cm
between passive and semi-passive DMFCs indicates the
oxygen mass transport limitation. It interesting to note that
the overall passive fuel cell performanceislimitedbyoxygen
mass transport and not that by PMTL. In semi-passive
DMFCs, a peak power density of 28 mWcm-2 is obtained,
which almost matches the performance of active DMFCs.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 608
Chart. 4: Comparative performance of passive and semi-
passive DMFCs
4. CONCLUSIONS
In a passive DMFC single cell, Nafion 115 membrane as a
PMTL has MTF of 4×10-4mL min-1 cm-2 controlled by
diffusion with 4M methanol solution. Peak power densities
of 21 and 28 mW cm-2 are obtained for passive and semi-
passive DMFCs, respectively. The performance obtained in
semi-passive DMFCs is comparable to that reported for
active DMFCs at ambient conditions.
REFERENCES
[1] W. Qian et al., “Architecture for portable direct liquid
fuel cells,” J. Power Sources, Vol. 154, Mar. 2006, pp.
202-213, doi: 10.1016/j.jpowsour.2005.12.019.
[2] A.S. Arico et al., “DMFCs: From Fundamental Aspectsto
Technology Development,” Fuel Cells, Vol. 1, Jul. 2001,
pp. 133-161, doi: 10.1002/1615-
6854(200107)1:2<133::AID-FUCE133>3.0.CO;2-5.
[3] L. Carrette et al., “Fuel Cells: Principles, Types, Fuels,
and Applications,” Chem. Phys. Chem., Vol.1,Dec.2000,
pp. 162-193, doi: 10.1002/1439-
7641(20001215)1:4<162::AID-CPHC162>3.0.CO;2-Z.
[4] Blum et al., “Water-neutral micro direct methanol fuel
cell (DMFC) for portable applications,” J. Power
Sources, Vol. 117, May. 2003, pp. 22-25, doi:
10.1016/S0378-7753(03)00310-0.
[5] C.Y. Chen and P. Yang, “Performance ofanair-breathing
direct methanol fuel cell,” J. Power Sources, Vol. 123,
Sep. 2003, pp. 37-42, doi: 10.1016/S0378-
7753(03)00434-8
[6] H. Chang et al., “Materials and processes for small fuel
cells” Solid State Ionics, Vol. 148, Jun. 2002, pp. 601-
606, doi: 10.1016/S0167-2738(02)00125-X.
[7] G.G. Park et al., “Pore size effect of the DMFC catalyst
supported on porous materials,” Int. J. Hydrogen
Energy, Vol. 28, Jun. 2003, pp. 645-650, doi:
10.1016/S0360-3199(02)00140-4.
[8] D. Kim et al., “Recent progress in passive direct
methanol fuel cells at KIST,” J. Power Sources., Vol.130,
May. 2004, pp. 172-177, doi:
10.1016/j.jpowsour.2003.12.023.
[9] W.M. Yang et al., “Effect of current-collector structure
on performance of passive micro direct methanol fuel
cell,” J. Power Sources., Vol. 164, Feb. 2007, pp. 549-
554, doi: 10.1016/j.jpowsour.2006.11.014.
[10] Y.H. Chan et al., “A self-regulated passive fuel-feed
system for passive direct methanol fuel cells,” J. Power
Sources, Vol. 176, Jan. 2008, pp. 183-190, doi:
10.1016/j.jpowsour.2007.10.050.
[11] M. Ali Abdelkareem and N. Nakagawa, “DMFC
employing a porous plate for an efficient operation at
high methanol concentrations,” J. Power Sources., Vol.
162, Nov. 2006, pp. 114-123, doi:
10.1016/j.jpowsour.2006.07.012.
[12] N. Nakagawa et al., “Control of methanol transport and
separation in a DMFC with a porous support,” J. Power
Sources, Vol. 160, Sep. 2006, pp. 105-115, doi:
10.1016/j.jpowsour.2006.01.066.
[13] M. Ali Abdelkareem and N. Nakagawa, “Effect ofoxygen
and methanol supply modes on the performance of a
DMFC employing a porous plate,”J.PowerSources.,Vol.
165, Mar. 2007, pp. 685-691, doi:
10.1016/j.jpowsour.2006.12.075.
[14] W.J. Kim et al, “Suppression of the methanol crossover
by hydrogels in passively operated flat-pack type
DMFCs and its application for the power source of
cellular phone,” J. Power Sources, Vol. 163, Dec. 2006,
pp. 98-102, doi: 10.1016/j.jpowsour.2006.05.048.
[15] W.J. Kim et al., “Hydrogels in methanol fuel cartridge
used as a diffusion-rate-controlling agent suppressing
the methanol crossover in passively operated flat-pack
type DMFCs,” J. Power Sources., Vol. 157, Jun. 2006, pp.
193-195, doi: 10.1016/j.jpowsour.2005.07.033.
[16] Y. Yang and Y.C. Liang, “A direct methanol fuel cell
system with passive fuel delivery based on liquid
surface tension,” J. Power Sources., Vol. 165, Feb. 2007,
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Passive DMFC with membrane diffusion of methanol

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 605 A passive DMFC with membrane for diffusion controlled methanol feed A. Balasubramanian1, R. Vijayakumar2 1Assistant Professor, Department of Petroleum Engineering, AMET University, Chennai – 603112, India 2Chemical Testing and Analytical Laboratory, Guindy, Chennai – 600 032, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Transport of methanol to the anode of a passive Direct Methanol Fuel Cell (DMFC) forvaryingconcentrationof methanol was studied using Nafion membranes of varying thickness namely, 50, 125, 175m. Themaximumpowerdensity was achieved with 1M aqueous methanol in the case of Nafion 112 as passive methanol transport layer (PMTL). Higher power density was achieved with 4M aqueous methanol while the power density decreased for concentrations higher than 4M in the case of Nafion 115 and Nafion 117. Maximumpower density of 21 mW cm-2 was obtained with Nafion 115 membrane as PMTL for 4M aqueous methanol at ambient conditions. Key Words: Passive Direct Methanol Fuel Cell; Transport; Methanol; Membranes; Power density. 1. INTRODUCTION Direct methanol fuel cells (DMFCs) have been an important area of research for application in portable electronic devices, such as notebook computers, personal digital assistants (PDAs), music systems and cellular telephones due to their advantages in terms of high energy density, simplicity and fast recharging [1-3]. However, in order to be commercially feasible, it is necessary to eliminate power losses from auxiliaries such as fuel and reactantfeed pumps, methanol and liquid level sensors, which are used in the active DMFCs. Passive DMFCs without such auxiliaries, have much simpler structures and are being investigated[4- 6]. Operating parameters and design of the passive DMFCs are crucial to enhance their performance. The operating parameters such as temperature, methanol flow rate and its concentration, and designaspectslikepassivemethanol feed system, CO2 removal from anode are mainly limiting the cell performance. The optimal methanol concentration was reported to be 4.0 M for passive DMFCs [7, 8]. Yang et al. [9] reported that much higher exposureratiooftheparallel flow field on the anode and perforated flow field on the cathode increased the delivery of fuel and oxygen, respectively resulting in enhanced performance. In passive DMFCs [10], higher temperature at cathode improves natural convection due to temperature difference between the MEA and the atmospheric air leading to enhanced performance. Presently, one of the most challenging problems for the passive DMFCs is supply of methanol at a desired flow rate and concentration from the reservoir tank to the anode. However, high and low methanol concentration lead to methanol crossover with resultant mixed potential on the cathode and low energy density, respectively [10]. Hence, some researchers [11-16] have made improvements in the fuel delivery system to increase the methanol feed concentration. Abdel kareem et al. [11-13] reported that while employing a porous carbon plate because of the increased mass transfer resistance higher concentration of methanol could be used. Kim et al. [14, 15] employed hydrogels in methanol fuel cartridges to control methanol diffusion rate from the fuel reservoir to the anode. Yangand Liang [16] reported on a DMFC system with passive fuel delivery based on liquid surface tension. In the present study, we report on the use of Nafion membrane of varying thickness as passive methanol transport layer (PMTL) for supply of methanol; in a diffusion-controlled mode to the anode. To the best of our knowledge, thiskindofapproachof passive delivery of methanol to the anode has not been reported. 2. EXPERIMENTAL Exploded view of passive DMFCs as shown in Fig. 1(A), was designed, fabricatedand tested in this study. The membrane electrode assembly (MEA) procured from M/s Johnson Matthey used in this study had 4 mg cm-2 loading of carbon- supported 1:1 Pt/Ru catalyst on the anode and 2 mg cm-2 loading of carbon-supportedPtonthecathode.ThisMEAwas sandwiched between anode and cathode graphite flow field plate, which was then clamped between two transparent acrylic fixture plates. Anode and cathode flow field plate machined into parallel windows and perforated holes, respectively. A step of 0.5 mm width and 0.5 mm depth was machined along the circumference of the parallel windows forremoval of CO2as shown in Fig. 1(B).Areservoirof5.0mL capacity was built in the anode fixture. 1M methanolsolution from the built-in reservoirwassuppliedtotheanodereaction zone through PMTL (Nafion 117 membrane) which was assembled between methanol reservoir tank and the anode flow field plate. Atmospheric air was supplied as an oxidant to the cathode reaction zone by natural convection. Bitrode T2000 electricalload interfacedtoacomputerwasemployed to record the voltage - current curves. The polarization curves were obtained in potentio static mode and discharge current was obtained at a constant voltage of 0.4V. At three current densities like 25, 50 and 75 mA cm-2 the concentration of CO2 gas (in ppm) was measured by using CO2 gas sensor (Vaisala CO2 sensor M170) as shown in Fig. 1 1(B). Similarlyelectrochemicalexperimentswerecarriedout with Nafion 115 and 112 membranes as PMTL for varying methanol concentration (1M, 2M, 3M, 4M and 5M).
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 606 Fig-1: (A) Schematic of exploded view of the passive DMFCs cell fixture. (B) Provision for CO2 removal in a passive DMFC 3. RESULTS AND DISCUSSION The amount of methanol delivery by passive feeding (diffusion) to reaction layer from reservoir is a function of methanol concentration and PMTL thickness that determines the cell performance. In Chart 2, the influence of the PMTL such as Nafion 112; Chart 2(A), Nafion 115; Chart 2(B), and Nafion 117; Chart 2(C) with varying methanol concentration (1M, 2M, 3M, 4M and 5M) on theperformance of passive DMFCs are given. In Chart 2 (A), it is clearly seen that higher performances at 1 and 2M while lower performances at 3, 4, and 5M methanol are obtained. With increase in methanol concentration increased methanol crossover resulted in decreased performance. Chart 2(C) shows that on replacement of PMTL i.e. Nafion 112 with Nafion 117, comparatively low performance at lower concentrations (1M and 2M) and enhanced performance at higher methanol concentrations (3M and 4M) are obtained, which is attributed to the decrease in methanol transport flux (MTF) due to increase in PMTL thickness from 50 to 175 m. Chart 2(B) shows the results obtained on replacement of PMTL i.e. Nafion 112 with 115. The polarization curves obtained for methanol concentrations 1M, 2M and 3M follow similar trend. A peak power density of 21 mW/cm-2 is obtained with 4.0 M methanol. However, in all cases with 5 M methanol, the OCVdecreased,indicating that significant methanol crossover from anode to cathode causes decrease in cell performance. The maximum power density is obtained for optimal passive methanol feeding by diffusion with PMTL using Nafion 115 membrane and 4M methanol. In passive DMFC single cell studies, the methanol crossover and methanol transportfluxareobtainedfromthe following equations. Initial volume in the reservoir Volume methanol crossed over Final volume in the reservoir Volume reacted            (1) Volume of methanol crossed over Volume of methanol used for oxidation Methanol Transport Flux Area of PMTL Time             (2) Chart. 1: Effect of passive methanol transport layer (A) Nafion 112, (B) Nafion 115 and (C) Nafion 117 membrane for varying methanol concentrations on performance of passive DMFCs.
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 607 Initial and final volume of methanol in the reservoir is noted for each test. Volume of methanol reacted is equivalent to faradaic oxidation of methanol. At constant current density of 40 mA cm-2, the methanol crossover current density and MTF are calculated using the above equations, for various methanol concentrations and for different PMTL and the data are shown in Chart 2. Increase in the thickness of the PMTL from 50 to 175 m leads to decrease in MTF thus limiting the mass transport to the anode and consequently, methanol crossover in passive DMFCs. Chart. 2: Methanol crossover current density (solid lines) and methanol transport flux (dotted lines) with respect to varying methanol concentrations at 40 mA cm-2. The concentrations of CO2 at 25, 50 and 75 mA cm-2 are 420, 500 and 590 ppm, respectively. It is interesting to note that the measured concentration in ppm corresponds to the faradaic oxidation of methanol. The discharge current behavior of the cell is also tested at varying methanol concentrations at a constant voltage of 0.4V with different PMTLs as shown in Chart 3. The discharge current density obtained for 5M concentration is less than that for 4M concentration reiterating the fact that MTF is optimal at 4M concentration. A maximum load current density of 33 mA cm-2 obtained with PMTL of Nafion 115 membrane at 4.0 M methanol can be attributed to the optimized PMTL and methanol concentration. Chart. 3: Discharge current density at a constant voltage (0.4V) with different passive methanol transport layers: (A) Nafion 112, (B) Nafion 115 and (C) Nafion 117 for varying methanol concentrations. In order to evaluate whether the passive DMFCs suffer from the oxygen mass transport limitation on the cathode, the limiting current density was measured with forced air on the cathode of a passive DMFC, also called as a semi-passive DMFC. Chart 4 shows the performance curve of passive and semi-passive DMFCs with optimized PMTL of Nafion 115 membrane and 4M methanol solution. In the performance curves, a difference in limiting current density of 15 mA cm between passive and semi-passive DMFCs indicates the oxygen mass transport limitation. It interesting to note that the overall passive fuel cell performanceislimitedbyoxygen mass transport and not that by PMTL. In semi-passive DMFCs, a peak power density of 28 mWcm-2 is obtained, which almost matches the performance of active DMFCs.
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 04 Issue: 07 | July -2017 www.irjet.net p-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 608 Chart. 4: Comparative performance of passive and semi- passive DMFCs 4. CONCLUSIONS In a passive DMFC single cell, Nafion 115 membrane as a PMTL has MTF of 4×10-4mL min-1 cm-2 controlled by diffusion with 4M methanol solution. Peak power densities of 21 and 28 mW cm-2 are obtained for passive and semi- passive DMFCs, respectively. The performance obtained in semi-passive DMFCs is comparable to that reported for active DMFCs at ambient conditions. REFERENCES [1] W. Qian et al., “Architecture for portable direct liquid fuel cells,” J. Power Sources, Vol. 154, Mar. 2006, pp. 202-213, doi: 10.1016/j.jpowsour.2005.12.019. [2] A.S. Arico et al., “DMFCs: From Fundamental Aspectsto Technology Development,” Fuel Cells, Vol. 1, Jul. 2001, pp. 133-161, doi: 10.1002/1615- 6854(200107)1:2<133::AID-FUCE133>3.0.CO;2-5. [3] L. Carrette et al., “Fuel Cells: Principles, Types, Fuels, and Applications,” Chem. Phys. Chem., Vol.1,Dec.2000, pp. 162-193, doi: 10.1002/1439- 7641(20001215)1:4<162::AID-CPHC162>3.0.CO;2-Z. [4] Blum et al., “Water-neutral micro direct methanol fuel cell (DMFC) for portable applications,” J. Power Sources, Vol. 117, May. 2003, pp. 22-25, doi: 10.1016/S0378-7753(03)00310-0. [5] C.Y. Chen and P. Yang, “Performance ofanair-breathing direct methanol fuel cell,” J. Power Sources, Vol. 123, Sep. 2003, pp. 37-42, doi: 10.1016/S0378- 7753(03)00434-8 [6] H. Chang et al., “Materials and processes for small fuel cells” Solid State Ionics, Vol. 148, Jun. 2002, pp. 601- 606, doi: 10.1016/S0167-2738(02)00125-X. [7] G.G. Park et al., “Pore size effect of the DMFC catalyst supported on porous materials,” Int. J. Hydrogen Energy, Vol. 28, Jun. 2003, pp. 645-650, doi: 10.1016/S0360-3199(02)00140-4. [8] D. Kim et al., “Recent progress in passive direct methanol fuel cells at KIST,” J. Power Sources., Vol.130, May. 2004, pp. 172-177, doi: 10.1016/j.jpowsour.2003.12.023. [9] W.M. Yang et al., “Effect of current-collector structure on performance of passive micro direct methanol fuel cell,” J. Power Sources., Vol. 164, Feb. 2007, pp. 549- 554, doi: 10.1016/j.jpowsour.2006.11.014. [10] Y.H. Chan et al., “A self-regulated passive fuel-feed system for passive direct methanol fuel cells,” J. Power Sources, Vol. 176, Jan. 2008, pp. 183-190, doi: 10.1016/j.jpowsour.2007.10.050. [11] M. Ali Abdelkareem and N. Nakagawa, “DMFC employing a porous plate for an efficient operation at high methanol concentrations,” J. Power Sources., Vol. 162, Nov. 2006, pp. 114-123, doi: 10.1016/j.jpowsour.2006.07.012. [12] N. Nakagawa et al., “Control of methanol transport and separation in a DMFC with a porous support,” J. Power Sources, Vol. 160, Sep. 2006, pp. 105-115, doi: 10.1016/j.jpowsour.2006.01.066. [13] M. Ali Abdelkareem and N. Nakagawa, “Effect ofoxygen and methanol supply modes on the performance of a DMFC employing a porous plate,”J.PowerSources.,Vol. 165, Mar. 2007, pp. 685-691, doi: 10.1016/j.jpowsour.2006.12.075. [14] W.J. Kim et al, “Suppression of the methanol crossover by hydrogels in passively operated flat-pack type DMFCs and its application for the power source of cellular phone,” J. Power Sources, Vol. 163, Dec. 2006, pp. 98-102, doi: 10.1016/j.jpowsour.2006.05.048. [15] W.J. Kim et al., “Hydrogels in methanol fuel cartridge used as a diffusion-rate-controlling agent suppressing the methanol crossover in passively operated flat-pack type DMFCs,” J. Power Sources., Vol. 157, Jun. 2006, pp. 193-195, doi: 10.1016/j.jpowsour.2005.07.033. [16] Y. Yang and Y.C. Liang, “A direct methanol fuel cell system with passive fuel delivery based on liquid surface tension,” J. Power Sources., Vol. 165, Feb. 2007, pp. 185-195, doi: 10.1016/j.jpowsour.2006.11.059.