Sheet Pile Wall Design and Construction: A Practical Guide for Civil Engineer...
Research plan 1
1. Research statement
August 16, 2015
(This article is based on what was posted on January 30, 2015, for Linkedin)
Toru Hara, PhD
Quest for Ultimate Energy Storage Device
1. Introduction and background
With supercapacitor-like rate capability and battery-like energy density, the energy storage
device can be the ultimate "one."
For the better rate capability, it is possibly known that the ideal electrode architecture is
three-dimensionally (3D) interpenetrated electron/ion network leading to efficient ion and electron
transport [1, 2]. For the higher energy density, active materials for batteries are formed in the 3D
architecture: Zhang et al. used electrodeposition to form NiOOH (cathode for nickel metal hydride
battery) and MnO2 (cathode for lithiµm-ion battery) electrodes directly onto 3D nickel current
collectors [3].
Battery that works in water-based (aqueous) electrolyte solutions, such as nickel metal
hydride batteries, has some advantages: (1) it does not need an inert atmosphere for manufacturing
unlike lithiµm-ion batteries thereby offering low cost; (2) it does not use flammable electrolyte
solutions unlike lithiµm-ion batteries thereby unlike lithiµm-ion batteries it does not catch a fire.
In contrast, the merit of lithiµm-ion batteries that work in organic electrolyte solutions is, they can
deliver higher output voltage because of greater electrochemical windows thereby offering high
energy density. So far the market seeking smaller and lighter batteries has been driving economy,
i.e., consumer electronics and lithiµm-ion batteries. From now onward, it is said that
environmental-protection-driven (= or energy-sustainability-driven) or security-of-materials-
driven (in a broad meaning) may drive economy. This may shed light on aqueous batteries,
particularly non-lithiµm-ion batteries: lithiµm is not abundant compared with sodium, proton, etc.
From this point of view, aqueous batteries with 3D-architectured electrodes, particularly Na+ or
H+ ion batteries can be promising.
2. Mono-atomic layer FeOOH / NiOOH battery
Among many candidates materials combinations, I have chosen (-) FeOOH / NiOOH (+).
The novelty is forming mono-atomic layers of FeOOH and NiOOH. The main objective is to elude
the beta-MOOH -> gamma-MOOH <-> alpha-M(OH)2 -> beta-M(OH)2 <-> beta-MOOH loop [M
= Fe, Ni] that can result in crystal structure destruction during charge/discharge. The phase change
is just a matter of the stacking pattern change [4]; the mono-atomic FeOOH and NiOOH layers
have no MOOH stacking thereby they can offer a long cycle life.
2. 2.1. FeOOH / NiOOH battery chemistry
At the anode (negative electrode) the following reaction takes place:
FeOOH + H+ + e- <-> Fe(OH)2, -0.56 V vs. SHE,
here, SHE denotes standard hydrogen electrode. Theoretical capacity is 301 mAh/g (470 mAh/g
is possible when overdischarged). Note that hydrogen evolution reaction can happen at -0.83 V vs.
SHE at pH = 14; thus, this side reaction can be suppressed even the anode is somewhat
overdischarged.
At the cathode (positive electrode) the following reaction takes place:
NiOOH + H+ +e- <-> Ni(OH)2, +0.49 V vs. SHE
Theoretical capacity is 292 mAh/g (467 mAh/g is possible when overcharged but usually
accompanying oxygen evolution side reaction). Note that oxygen evolution reaction can happen
at 0.4 V vs. SHE at pH = 14 although the overpotential of the reaction may be expected to some
extent.
The full cell reaction becomes
NiOOH + Fe(OH)2 <-> Ni(OH)2 + FeOOH, Ecell = 1.05 V.
This battery eliminates a slow reaction of the conventional NiFe battery reaction: that is
2NiOOH + Fe + 2H2O <-> 2Ni(OH)2 + Fe(OH)2, Ecell = 1.37 V. This battery only uses the second
reaction of the conventional NiFe battery: NiOOH + Fe(OH)2 <-> Ni(OH)2 + FeOOH, Ecell = 1.05
V. Recently, many researchers are trying to use nanosized iron oxide as the anode instead of metal
iron, e.g., Fe2O3 [5] or Fe3O4 [6]; however, the redox reactions via iron oxides tend to be
irreversible or slow.
2.2. 3D interpenetrated electron/ion network for mono-atomic layer FeOOH / NiOOH battery
In order to form 3D interpenetrated electron/ion network, 3D current collector can be used.
There are various types of 3D current collectors; among them graphene paper is a promising
candidate. Suppose 30 mg/cm2 (corresponding to 9 mAh/cm2) of FeOOH is directly deposited onto
current collectors:
(1) metal foil, surface area =1.0 cm2 (real)/cm2 (nominal), FeOOH thickness = 211 µm;
(2) carbon fiber paper [e.g., TGP-H-60 (Toray Industry Inc., 190-μm thick)], surface area = 33.4
cm2 (real)/cm2 (nominal), FeOOH thickness = 6.3 µm;
(3) activated carbon fiber paper (e.g., 190-µm thick), surface area = 3 340 cm2 (real)/cm2 (nominal),
FeOOH thickness = 63 nm;
3. (4) carbon-fiber-paper-supported carbon nanofoam (e.g., 190-µm thick); surface area = 64 000
cm2 (real)/cm2 (nominal), FeOOH thickness = 3.3 nm;
(5) graphene paper (e.g., 200-µm thick), surface area = 2630 m2/g x 16 mg/cm2 = 420 800 cm2
(real)/cm2 (nominal), FeOOH thickness = 0.50 nm;
(6) reduced graphene oxide & carbon nanotube paper [7], surface area = 651 m2/g x 16 mg/cm2
(supposing a thickness of around 200 µm) = 104 160 cm2 (real)/cm2 (nominal), FeOOH thickness
= 2.0 nm.
There can be a less expensive 3D current collector: (i) starting from Ni foam, NiSn intermetallic
layer is electrodeposited onto theNi foam; (ii) next, Sn is dissolved into alkaline solution,
remaining porous Ni layer.
2.3. FeOOH- and NiOOH-forming onto 3D current collector
There are two options regarding the FeOOH- and NiOOH-forming process, chemical
synthesis and electrodeposition. I have chosen electrodeposition.
Particularly when using graphene, chemical synthesis tends to result in a dot-on-graphene
structure or a multi-atomic MOOH layer [8,9]. Electrodeposition is promising even though mono-
atomic layer formation has not been reported so far [3, 10-13]. Particularly, pulse electrodeposition
at a high current density is preferable.
2.4. Electron (or hole) conductivity of FeOOH and NiOOH
The reduced forms of active materials, M(OH)2 are highly insulating: Ni 3d-t2g orbitals are
relatively well hybridized with O 2p orbitals; however, it is not the case with Fe 3d-eg orbitals.
Thus mono-atomic thick MOOH is preferable particularly for FeOOH.
2.5. Other anode materials choices
Besides NiFe battery, NiOOH cathode has been used with various types of anode materials
such as Zn, Cd, metal hydride, etc.
As for Zn anode, the current problems are inefficient zinc utilization and internal short
circuit failure resulting from zinc dendrite formation. In order to improve zinc utilization and to
suppress zinc dendrite formation, a redesign of zinc electrode will be required, i.e., a porous,
monolithic, 3D aperiodic architecture [14, 15]: according to the authors of refs. 14 and 15, the
redesigned Zn sponge electrode provides (i) an inner core of Zn that is retained throughout battery
charge/discharge to facilitate long-range electronic conductivity, (ii) amplification of electrified
interfaces to distribute current uniformly throughout the electrode structure, and thus eliminate
dendrite forming high current densities, and (iii) confined void volume elements within the interior
of the porous anode that expedite saturation/dehydration of zincate to ZnO, thus preventing shape
4. change. However, the Zn sponge electrode may be difficult for scaling up electrode size. The same
functions can be offered by directly electrodepositing Zn onto 3D current collector (I already
initiated one R&D project on Zn/NiOOH battery).
Cadmium is not a choice because of its toxicity.
Metal hydride may survive: Kawasaki Heavy Indutry delivers 30-year-life nickel metal
hydride battery, Gigacell.
Zn still has a strength regarding its energy density: it delivers the most negative potential
and the highest theoretical capacity among anode materials that can be used in aqueous media.
Note that NiZn battery is a hybrid ion system (Zn2+ and H+) like Leclanche cell or alkaline
manganese cell.
There may be other choices.
Vanadium oxide may not be a choice since it is lethally toxic.
MoO3 is not cheap and the supply can be restricted. Molybdenum, country of origin: 1.
China (104 000 ton/year), 2. USA (60 400), 3. Chile (35 090), 4. Peru (16 790), 5. Mexico (11
000) up, 6. Canada (9 005), 7. Iran (6 300), 8. Turkey (5 000), 9. Armenia (4 900), 10. Russia
(3,900), 11. Mongol (1,903), 12. Uzbekistan (550). Molybdenum, amount of deposit: 1. China (4
300 000 ton), 2. USA (2 700 000), 3. Chile (1 100 000), 4. Peru (450 000), 5. Russia (250 000), 6.
Armenia (200 000), 7. Canada (200 000), 8. Mongol (160 000), 9. Mexico (130 000), 10.
Kazakhstan (130 000), 11. Kyrgystan (100 000), 12. Uzbekistan (60 000), 13. Iran (50 000).
Uneven distribution of countries of origin has often generated international friction. In addition,
molybdenum is a key material for various types of specialty steel. The omnipresence of raw
materials is one of key requirements for supplying cheap batteries.
Surface-modified carbon-based materials such as HNO3 treated carbon nanotubes and/or
graphene oxide can be candidate alternatives. In order to re-obtain the electronic conductivity of
above-mentioned carbonaceous materials, a mild reduction process (resulting in O content = 10-
15%) such as a heat treatment at 200-250 degrees Celsius in an inert atmosphere is preferable than
harsh chemical reduction processes since oxygen-based functional groups are required in order to
obtain a high capacity in aqueous media. However, gravimetric capacities of the above-mentioned
materials tend to be not high enough. It has been known that Russian companies, ELTON (ESMA),
delivers asymmetric electrochemical capacitors, (-) activated carbon / NiOOH (+): carbon
nanotube- or graphene-based materials can be good alternatives for activated carbon.
2.6. Other cathode materials choices
In Leclanche cells and alkaline manganese cells, MnO2 is used as the cathode material (I
prefer the expression, MnOOH, since I consider that it should be clearly described as a proton
intercalation/deintercalation material). The problems are a relatively low gravimetric capacity
(usually 100-150 mAh/g is available) and dissolution into aqueous media because of the multi-
5. valency of manganese. It is noteworthy that MnO2 can be directly electrodeposited onto current
collectors [3].
3. Practical issues
3.1. Oxygen evolution at NiOOH cathode
While charging, oxygen gas may evolve at the NiOOH cathode. The overpotential of
oxygen evolution at pure NiOOH electrode can be +0.23 V in 1 M KOH solution at 10 mA/cm2
[16,17], for example. Since the electrical conductivity of Ni(OH)2/NiOOH is not high (101 - 106
Ω/cm) [18-21] (cf. FeOOH, 105 - 107 Ω/cm [22,23]), thick NiOOH films tend to suffer from
overlap of its redox potential with oxygen evolution potential because of a high internal resistance
(therefore, hole doping such as Co2+/3+ doping is often carried out); however, it is not the case with
mono-atomic layer NiOOH on graphene sheet. Instead, the pH of electrolyte solution (by
decreasing the concentration of KOH, oxygen evolution potential becomes more positive thereby
oxygen cannot start evolving until reaching a more positive potential.), a relatively low oxygen
evolution overpotential at a low current (meaning that oxygen starts evolving at a less positive
potential when the battery is operated at a low C-rate) must be taken into consideration.
Although I am not going to dope Co2+/3+ into NiOOH for this mono-atomic layer FeOOH
/ NiOOH battery, it might be interesting to investigate the doping effect on the mono-atomic layer
NiOOH or FeOOH when considering the electron/hole conduction modulation by internal
hole/electron doping and by ad-atom or ad-ion surface doping [24-27].
3.2. Electrochemical impedance spectroscopy (EIS)
Since mono-atomic layer FeOOH / NiOOH battery has a great surface area particularly
when deposited onto graphene paper, thereby has a great capacity (the response speed limit may
still be a mere 1000 C corresponding to 0.36 s, though), and since a few layers of graphene and
FeOOH or NiOOH can have a so-called quantum capacitance (In addition, graphene oxide,
FeOOH, and NiOOH may exhibit current relaxation that is related to charge trapping/detrapping
into/from defective states or their genuine 3d orbitals [28-30]: this relaxation is also a redox
reaction.), I may not recommend EIS to explore the underlying rate-determining step(s) because
of its high CR time constant etc. [C denotes capacitance that is the sum of electrical double layer
capacitance and pseudo-capacitance, R denotes series equivalent resistance (SER)] (Note that SER
does not mean DC resistance or a resistance at the lowest frequency; if one wants to analyze charge
transfer process etc., one must use the impedance value at the intersection with the real axis.).
4. Future prospects
6. Considering the possibility of 9 mAh/cm2 with an electrode thickness of 200 µm (assuming
a mass-loading of 30 mg/cm2), the mono-atomic layer FeOOH/NiOOH battery deposited onto 3D
graphene papers can be competitive enough with lithium-ion batteries that usually offers around
2.5 mAh/cm2 with an electrode thickness of 100 µm although its output voltage of 1 V is lower
than that of lithium-ion batteries, 3.6 V. Furthermore, eluding the β-MOOH -> γ-MOOH <-> α-
M(OH)2 -> β-M(OH)2 <-> β-MOOH loop [M = Fe, Ni] [4] by forming mono-atomic layer can
lead to a super long cycle life that has not been realized: this can be called a 0.5-step beyond the
cutting edge.
However, a practical compromise or a 1-step-beyond-the-cutting-edge technology may be
required since conventional batteries performance has been improved year by year.
4.1. Compromise for increasing volumetric capacity
In order to increase the volumetric capacity, a few to several atomic layer thick FeOOH
and NiOOH electrodes may be preferred.
4.2. One step beyond the cutting edge
By taking full advantage of the 3D architecture and the combination of mono-atomic layer
active materials, even all-solid-state energy storage device with a practically high enough
capacity/pseudo-capacitance may be possible. In that case, redox reactions should be re-considered
the current relaxation that is charge trapping/detrapping into/from defective states or genuine 3d
orbitals [28-30] etc.
References
[1] J. W. Long, B. Dunn, D. R. Rolison, H. S. White, Chem. Rev. 104 (2004) 4463-4492.
[2] D. R. Rolison, J. W. Long, J. C. Lytle, A. E. Fischer, C. P. Rhodes, T. M. McEvoy, M. E. Bourga, A. M. Lubersa,
Chem. Soc. Rev. 38 (2009) 226-252.
[3] H. Zhang, X. Yu, P. Braun, Nat. Nanotechnol.6 (2011) 277-281.
[4] H. Bode, K. Dehmelt, J. Witte, Electrochim. Acta, 11 (1966) 10791087.
[5] J. Liu, M. Chen, L. Zhang, J. Liang, J. Yan, Y. Huang, J. Lin, H. J. Fan, Z. X. Shen, ACS Nano Lett. 14 (2014)
7180-7187.
[6] T. W. Lin, C. S. Dai, K. C. Hung, Scientific Reports 4 (2014) 7274, DOI: 10.1038/srep07274.
[7] W. Han, Y. E. Miao, Y. Huang, W. W. Tiju, T. Liu, RSC Adv.,5 (2015) 9228-9236.
[8] C. Peng, B. Jiang, Q. Liu, Z. Guo, Z. Xu, Q. Huang, H. Xu, R. Tai, C. Fan, Energy Environ. Sci., 4 (2011) 2035-
2040.
[9] Y. Sun, X. Hu, W. Luo, H. Xu, C. Hu, Y. Huang, ACS Appl. Mater. Interfaces, 5 (2013) 10145-10150.
7. [10] L. Huang, D. Chen, Y. Ding, S. Feng, Z. L. Wang, M. Liu, Nano lett. 13 (2013) 3135-3139.
[11] G. R. Fu, Z. A. Hu, L. J. Xie, X. Q. Jin, Y. L. Xie, Y. X. Wang, Z. Y. Zhang, Y. Y. Yang, H. Y. Wu, Int. J.
Electrochem. Sci. 4 (2009) 1052-1062.
[12] L. Gu, Y. Wang,R. Lu, L. Guan, X. Peng, J. Sha, J. Mater. Chem. A, 2 (2014) 7161-7164.
[13] S. Jiao, L. Xu, K. Hu, J. Li, S. Gao, D. Xu, J. Phys. Chem. C, 114 (2010) 269-273.
[14] J. F. Parker, C. N. Chervin, E. S. Nelson, D. R. Rolison, J. W. Long, Energy Environ. Sci. 7 (2014) 1117-1124.
[15] J. F. Parker, E. S. Nelson, M. D. Wattendorf, C. N. Chervin, J. W. Long, D. R. Rolison. ACS Appl. Mater.
Interfaces, DOI: 10.1021/am505266c.
[16] J. R. Swierk, S. Klaus, L. Trotochaud,A. T. Bell, T. D. Tilley, J. Phys.Chem. C, DOI: 10.1021/acs.jpcc.5b05861.
[17] S. Klaus, Y. Cai, M. W. Louie, L. Trotochaud,A. T. Bell, J. Phys. Chem. C 119 (2015) 7243-7254.
[18] H. Kamal, E. K. Elmaghraby, S. A. Ali, K. Abdel-Hady, J. Cryst. Growth, 262 (2004) 424-434.
[19] U. M. Patil, K. V. Gurav, V. J. Fulari, C. D. Lokhande, J. Power Sources, 188 (2009) 338-342.
[20] H. Ueta, Y. Abe, K. Kato, M. Kawamura, K. Sasaki, H. Itoh, Jpn. J. Appl. Phys. 48 (2009) 015501.
[21] N. D. Koshel, V. V. Malyshev, Surf. Engin. Appl. Electrochem. 46 (2010) 348-351.
[22] M. S. Burke, M. G. Kast, L. Trotochaud, A. M. Smith, S. W. Boettcher, J. Am. Chem. Soc. 137 (2015) 3638-
3648.
[23] D. Chen, M. Yen, P. Lin, S. Groff, R. Lampo, M. McInerney, J. Ryan, Materials 7 (2014) 5746-5760.
[24] T. Hara, K. Shinozaki, Jpn. J. Appl. Phys.50 (2011) 065807.
[25] T. Hara, T. Ishiguro, K. Shinozaki, Jpn. J. Appl. Phys.49 (2010) 041104.
[26] T. Hara, T. Ishiguro, N. Wakiya, K. Shinozaki, Mater. Sci. Eng. B 161 (2009) 142-145.
[27] T. Hara, T. Ishiguro, N. Wakiya, K. Shinozaki, Jpn. J. Appl. Phys. 9 (2008) 7486-7489.
[28] T. Hara, Microelectron. Eng. 75 (2004) 316-320.
[29] T. Hara, Solid State Commun. 132 (2004) 109-114.
[30] T. Hara, Mater. Chem. Phys. 91 (2005) 243-246.