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Review

How Close We Are to Achieving Commercially Viable Large-Scale Photobiological Hydrogen Production by Cyanobacteria: A Review of the Biological Aspects

1
Research Institute for Photobiological Hydrogen Production, Kanagawa University, Tsuchiya, Hiratsuka, Kanagawa 259-1293, Japan
2
The OCU Advanced Research Institute for Natural Science and Technology (OCARINA), Osaka City University, 3-3-138 Sugimoto, Sumiyoshi-ku, Osaka 558-8585, Japan
3
Department of Biological Sciences, Kanagawa University, Tsuchiya, Hiratsuka, Kanagawa 259-1293, Japan
*
Author to whom correspondence should be addressed.
Life 2015, 5(1), 997-1018; https://doi.org/10.3390/life5010997
Submission received: 5 January 2015 / Revised: 16 February 2015 / Accepted: 9 March 2015 / Published: 18 March 2015
(This article belongs to the Special Issue Cyanobacteria: Ecology, Physiology and Genetics)

Abstract

:
Photobiological production of H2 by cyanobacteria is considered to be an ideal source of renewable energy because the inputs, water and sunlight, are abundant. The products of photobiological systems are H2 and O2; the H2 can be used as the energy source of fuel cells, etc., which generate electricity at high efficiencies and minimal pollution, as the waste product is H2O. Overall, production of commercially viable algal fuels in any form, including biomass and biodiesel, is challenging, and the very few systems that are operational have yet to be evaluated. In this paper we will: briefly review some of the necessary conditions for economical production, summarize the reports of photobiological H2 production by cyanobacteria, present our schemes for future production, and discuss the necessity for further progress in the research needed to achieve commercially viable large-scale H2 production.

1. Introduction

1.1. Global Climate Change

The concentration of atmospheric CO2 has been increasing since the era of the industrial revolution when it was estimated to be 270–280 ppm initially, rising to current levels of about 400 ppm. According to the fifth assessment report of the UN IPCC (United Nations Intergovernmental Panel on Climate Change) [1,2], the greatest contribution to the global increase in greenhouse gases comes from CO2 emitted by burning fossil fuels (65%) and land use changes (deforestation) (11%), followed by methane (16%), N2O (6%) and fluorocarbons, etc. (2%). Currently, the amounts of greenhouse gases emitted have continued to rise due to the increases in human activities and population growth. If we are able to stabilize the atmospheric greenhouse gases at 530–580 ppm-CO2 equivalent (approximately twice that of the pre-industrial level), one of the ICPP scenarios predicts that we will need to reduce global greenhouse gas emissions by 19%–47% in 2050 and 59%–81% in 2100 (relative to 2010 emissions) (Figure 1). Some scenarios predict that we will need to go beyond reduction strategies and achieve “negative emissions” by CO2 sequestration, etc. Economically advanced countries will likely be required to reduce emissions the most, perhaps by as much as 80% compared to present levels. Even if we succeed in stabilizing greenhouse gases at the level of 530–580 ppm CO2 equivalent, the global average temperature will rise around 2.0–2.2 °C relative to the 1850–1900 temperatures. Stabilizing emissions at a less-stringent level of 720–1000 ppm-CO2 equivalent, would still require substantial emissions reduction from current, largely unregulated levels, and result in the average temperature rising around 3.1–3.7 °C relative to the 1850–1900 temperatures. From all of these considerations, it is evident that we urgently need viable renewable energy technologies as part of a global strategy to drastically reduce CO2 emissions from burning fossil fuels and thus avert potentially catastrophic climate change.
Figure 1. Some scenarios for annual greenhouse gas (GHG) emission, UN IPCC. Due to uncertainty regarding future emissions and prediction of the outcome, probable ranges are shown for each stabilization targets. Stabilization at 530–580 and 720–1000 ppm CO2-eq respectively in 2100. The upper level of the probable range of >1000 ppm CO2-eq line in IPCC scenario is also shown. (Adapted from Figure SPM4, IPCC, 2014: Summary for Policy Makers, the Climate Change 2014 [1]).
Figure 1. Some scenarios for annual greenhouse gas (GHG) emission, UN IPCC. Due to uncertainty regarding future emissions and prediction of the outcome, probable ranges are shown for each stabilization targets. Stabilization at 530–580 and 720–1000 ppm CO2-eq respectively in 2100. The upper level of the probable range of >1000 ppm CO2-eq line in IPCC scenario is also shown. (Adapted from Figure SPM4, IPCC, 2014: Summary for Policy Makers, the Climate Change 2014 [1]).
Life 05 00997 g001

1.2. Prospects for Large-Scale Algal Biofuel Production

We are currently consuming energy at an unsustainably high rate, with much of the consumption (about 82%) coming from fossil fuels (Table 1) (International Energy Agency (IEA), IEA 2014) [3]. Land-based production of biofuels has been proposed to meet at least some of our energy needs. One method for assessing the energy potential of land-based production systems is to consider total primary energy consumption in the context of the nutritional energy consumption largely derived from current land-based crop systems. In terms of total primary energy consumption, on a world-wide average, people consume about 25 times their nutritional energy (20 times, compared with the fossil fuel-derived energy) (Table 1): people in US 100, Germany 56, Japan 52, China 31 times, respectively (IEA Energy Indicators 2012 in (IEA Key World Energy Statistics 2014)) [4]. From this comparison, it is evident that we cannot expect much more additional energy from land-based agricultural crops, such as sugar cane and corn. Accordingly, there are growing interests in the development and production of biofuels, such as biomass, biodiesel, and H2, using a variety of microalgae grown on lands that are not suitable for agricultural production [5,6,7,8,9]. However, commercially viable large-scale fuel production from microalgae has yet to be realized.
Table 1. Solar energy and human energy consumption.
Table 1. Solar energy and human energy consumption.
Energy Intensity and QuantityRatiosRefs./Remarks
Solar energy received on Earth surface
 Intensity165 W·m−2 (1450 kWh·m−2·yr−1) [10]
 Total energy2,660,000 × 1018 J·yr−147505800440,000[10]
 Photosynthetically active radiation1,200,000 × 1018 J·yr−1 45% of the total
Human social energy consumption
 Total primary energy supply560 × 1018 J·yr−111.2225[3]
 Fossil fuel consumption460 × 1018 J·yr−10.82121[3]
 Human digestive energy intake22 × 1018 J·yr−10.0390.0481Population: 7.2 × 109
2000 kcal·capita−1·day−1

1.3. Examples of Policies to Promote the Development of Renewable Energy Technologies

1.3.1. Feed-In Tariff Scheme in Germany

Feed-in electricity tariffs were introduced in Germany in 2004 to encourage the use of new energy technologies, such as wind, hydro- and geo-thermal power, biomass, and solar photovoltaics. Feed-in tariffs are a policy employed by governments to encourage investment in renewable energy technologies by providing them a fee (or “tariff”) above the retail rate of electricity. Feed-in tariffs provide long-term investment security to renewable energy producers and are typically based on the costs of specific technology. Wind power, for instance, costs less to produce than solar PV or tidal powers, so the tariff awarded is correspondingly lower. In a Wikipedia entry [11], the German feed-in tariff system is described as one of the most efficient and effective support schemes in the world for promoting renewable electricity. As of August 2014, a revised Renewable Energy Sources Act (EEG 2014, also called EEG 2.0) was implemented in Germany, with some modifications to the feed-in tariffs. The aim is to meet Germany’s renewable energy goals of 40% to 45% of electricity consumption in 2025 and 55% to 60% in 2035 [12].
For an international comparison of the price of energy and feed-in tariff, the following currency exchange rates (approximate average currency exchange rates in 2014) were assumed in this paper: 1 Euro = 132 US¢, and 100 Japanese Yen = 94 US¢. The German feed-in tariffs in August of 2014 are: 4.62 US¢/kWh for hydropower facilities up to 50 MW, 16.5 ¢/kWh for those up to 500 kWh, 16.4 ¢/kWh for solar installations on buildings up to 10 kW and 25.6 ¢/kWh for offshore wind [12]. The tariffs for photovoltanics in 2014 decreased by about 80% compared with those in 2004, the starting year of the German program, demonstrating the effectiveness of the policy strategy.

1.3.2. Feed-In Tariff Scheme in Japan [13]

The government of Japan introduced feed-in tariffs in 2012. In April 2014, the purchase prices (excluding the tax, with the purchase period of 10 or 20 years at fixed prices) were: 34.8 ¢/kWh for photovoltanics up to 10 kWh, 30.1 ¢/kWh for those 10 kW or more, 20.7 ¢/kWh for land-based wind power, 33.8 ¢/kWh for offshore wind power, and 13.2 ¢/kWh for medium hydropower. Because the prices offered by the government were so favorable to investors, in southern Japan, Kyushu Electric Power Co. had to suspend receipt of applications from large-sized renewable-energy producers (photovoltanics) wishing to access the company’s grid while it reviews how much more clean energy it’s capable of handling on sunny days.

1.3.3. Estimated Cost of Electricity in the USA

According to the 2012 estimates by the US Energy Information Administration (eia), the levelized cost of electricity in ¢/kWh for plants entering service in 2019 are: conventional coal 9.56 (no subsidy), geothermal 4.79 (4.45, with subsidy), solar photovoltanic 13.0 (11.86 with subsidy), etc. [14]. These estimates illustrate that for the US, coal continues to be a relatively cheap source of electricity even though burning coal emits a large amount of CO2 into the atmosphere. In order to decrease CO2 emissions from coal, the integrated coal-gasification combined cycle (IGCC) (estimated to be 11.59 ¢/kWh) and IGCC with carbon control and sequestration (CCS) systems have been proposed (estimated to be 14.74 ¢/kWh). The CO2 captured in these systems is transported to a storage site, normally an underground geological formation. The effectiveness of CCS, and its long-term effects on the environment need to be carefully assessed.

1.3.4. Possible Merit of H2 as Motor Fuels

The next-generation of fuel-efficient cars is entering the consumer market. Toyota recently announced the commercialization of hydrogen fuel-cell vehicles called “Mirai” in December 2014 [15]. According to Toyota, using measurements based on the Japanese JC08 test cycle, a cruising range of approximately 700 km can be achieved when fueled with H2 at 70 MPa. In comparison, the cruising ranges of electric cars might be around 100–200 km per full battery charge. In the same month, several Japanese gas companies announced opening commercial hydrogen refueling stations with the introductory prices of H2 (subsidized by the government) ranging from 9.4 to 10.3 US$ (1000–1100 Japanese Yen) per kg, or 23.8–26.1 ¢/kWh [16]. Because the energy efficiency of fuel cell cars is better than internal combustion engine cars, it is estimated that H2 fuel will be competitive with gasoline 1.22–1.60 US$/L (retail price of about 13.9–18.3 ¢/kWh including tax, calculated on an energy density of 8.76 kWh/L).

2. Outline of the Biological Processes of Photobiological H2 Production by Heterocyst-Forming Cyanobacteria

Photobiological production of biomass by photosynthetic organisms (trees, grasses, algae, etc.) is considered one of the better candidates for large-scale, renewable energy because the amount of solar energy is almost infinite (Table 1). Photobiological H2 production by cyanobacteria is one of the options, and this review briefly discusses nitrogenase (N2ase)-based photobiological H2 production by cyanobacteria because it is the focus of our current studies. In doing so, we do not intend to supplant other systems, such as hydrogenase (H2ase)-based photobiological H2 production by various algae including cyanobacteria, as well as biofuel production (e.g., biomass, biodiesel) by various photosynthetic microorganisms.
Some strains of cyanobacteria possessing N2ase are good candidates for optimization of photobiological H2 production [17,18,19,20,21]. N2ase catalyzes the following reaction under optimal conditions for N2 fixation:
N2 + 8 e + 8 H+ + 16 ATP → H2 + 2 NH3 + 16 (ADP + Pi)
whereas, in the absence of N2 (e.g., under Ar), all es are allocated to H2 production:
2 e + 2 H+ + 4 ATP → H2 + 4 (ADP + Pi)
The above reactions catalyzed by N2ase are essentially irreversible. N2ase is extremely O2 sensitive and quickly inactivated by O2. In order to reconcile the activities of the O2-sensitive N2ase with O2-evolving photosynthesis, cyanobacteria have evolved various means to address to the physiological challenges [22]. There are three basic groups. In Group 1, the two processes are separated spatially as found in heterocystous filamentous types (e.g., Anabaena, Nostoc, Calothrix). In Group 2, the processes are separated temporally by circadian rhythm as found in non-heterocystous unicellular and filamentous types (e.g., Cyanothece, Lyngbya). In Group 3, other non-heterocystous filamentous types (e.g., Trichodesmium) seem to sporadically perform the two processes: some of the cells have ordinary O2-evolving photosynthesis activity, while the others temporally cease photosynthesis and fix N2 [23].
In this review, we will discuss mainly Group 1 cyanobacteria, as these strains are the focus of our research and because they are the most extensively studied among the three groups with respect to physiology, molecular biology, etc. [24,25,26]. The cells are organized as filaments, with the majority of the cells (called vegetative cells) synthesizing organic compounds by ordinary photosynthesis. Under combined-nitrogen deficiency a few of the cells develop into heterocysts, cells specialized for nitrogen fixation. Heterocysts lacking photosystem II activity, have increased respiration and are surrounded by a thick cell envelope that impedes the entry of O2, thus providing a micro-oxic environment to protect the N2ase from inactivation by O2. They receive saccharides from neighboring vegetative cells and the saccharides are then used as the electron donors for the N2ase reaction (Figure 2). Within heterocysts, photosystem I reduces low-potential ferredoxin and/or flavodoxin and contributes to the generation of ATP through photophosphorylation. The fixed nitrogen is converted to glutamine, which is transported to vegetative cells. In this manner, heterocystous cyanobacteria are able to simultaneously perform O2-evolving photosynthesis and the O2-labile N2ase reaction.
Many of these types of cyanobacterial strains have the uptake hydrogenase (Hup) and some (but not all) of them also have the bidirectional hydrogenase (Hox) [27,28,29]. The former H2ase reabsorbs H2 produced by N2ase and thus the presence of Hup activity can limit the net production of H2 by the N2ase. There has been a report of an environmental isolate of the non-heterocystous Oscillatoria sp. strain Miami BG7 that lacks Hup activity and is able to accumulate H2 in the presence of photosynthetically evolved O2 [30]. When Hup activity was eliminated by molecular genetic techniques [28,31,32,33,34,35,36] or chemical mutagenesis [37], the resulting cyanobacterial mutants showed enhanced H2 production activity. Since in contrast to H2ase activity, N2ase catalyzes an essentially unidirectional H2 production and thus does not consume H2, cyanobacterial mutants lacking Hup activity are able to accumulate H2 to about 7%–30% (v/v) in the presence of O2 evolved [35,38].
Figure 2. Outline of H2-related metabolic routes in heterocyst-forming cyanobacteria. Vegetative cells synthesize saccharides (CH2O) by ordinary photosynthesis with accompanying evolution of O2 and uptake of CO2. Heterocysts receive the saccharides, and use them (accompanied by CO2 evolution) as the sources of e for N2ase reaction. For efficient net production of H2, H2ase(s) (uptake H2ase Hup and bidirectional H2ase Hox) have been inactivated. C6P: hexose phosphate, Fdox and Fdred: ferredoxin oxidized and reduced respectively, OPPP: oxidative pentose phosphate pathway, PSI and PSII: photosystem I and II, respectively (adapted from [21] with modification).
Figure 2. Outline of H2-related metabolic routes in heterocyst-forming cyanobacteria. Vegetative cells synthesize saccharides (CH2O) by ordinary photosynthesis with accompanying evolution of O2 and uptake of CO2. Heterocysts receive the saccharides, and use them (accompanied by CO2 evolution) as the sources of e for N2ase reaction. For efficient net production of H2, H2ase(s) (uptake H2ase Hup and bidirectional H2ase Hox) have been inactivated. C6P: hexose phosphate, Fdox and Fdred: ferredoxin oxidized and reduced respectively, OPPP: oxidative pentose phosphate pathway, PSI and PSII: photosystem I and II, respectively (adapted from [21] with modification).
Life 05 00997 g002
In the unicellular diazotrophic cyanobacterium Cyanothece sp. strain PCC 7822, the N2ase and H2 production activities are inactivated following disruption of the hupL gene (encoding a large subunit of Hup) via molecular genetic techniques, indicating that Hup protects N2ase from oxygen toxicity by removing O2 in this strain [39].
Although Hup may play such a role, the degree of its N2ase protection may differ among strains, and we can selectively use the strains (either heterocystous or unicellular) in which the negative effects of elimination of Hup on net H2 production are low.

3. Some Lessons from Studies of the Economics of Large-Scale Algal Fuel Production

3.1. Benemann’s Critical View of Algal Biofuel Production

Benemann has been studying photobiological biofuel production by various algae, since the first discovery of N2ase-based photobiological H2 production by cyanobacteria [40]. He critically examined the viability of microalgae for the production of gaseous fuels, specifically H2 and CH4, and assessed various proposed schemes on the basis of their technological and economic feasibility. In 2004, he summarized his opinion [41] as: “Processes for the production of gaseous fuels, H2 and CH4, using microalgae culture have been studied from a scientific perspective for several decades, and the practical cultures have been studied relatively recently. The lack of practical results in H2 and CH4 production cannot be ascribed to limited R&D funding. The only present practical application is the harvesting of algal biomass from wastewater treatment ponds by chemical flocculation, followed by the anaerobic digestion of the algal biomass. Overall, costs of such a process were estimated at about $10 per GJ of H2 (3.6 ¢/kWh).” Benemann’s conceptual steps for a techno-economic analysis consisted of: (1) Production in open ponds (costing $7 m−2, 0.5 km2 in area in some of his analyses), at a solar efficiency of 10%, of a nitrogen-limited biomass (that accumulates large amounts of storage carbohydrates); (2) Concentration of the biomass from the ponds in a settling pond; (3) Anaerobic dark fermentation to yield 4 H2/glucose stored in the algal cells, plus two acetate moles; and (4) Reaction in a photobioreactor in which the algal cells would be converted from the two acetate moles to eight moles of H2. The cost of the process was estimated at about $10 per·GJ−1 of H2, (3.6 ¢/kWh) with the photobioreactor comprising about half of the total cost. In our opinion, a photosynthesis efficiency of 10%, required for economical production, is very difficult to attain even if an algal H2ase serving as a highly efficient H2 catalyst is used.

3.2. Life-Cycle Analysis (LCA) of the Energy Requirements for Algal Fuel Production

Clarens et al. [42] made LCA analyses of biofuel production by microalgae based on published records (first-generation algae production), and found that algae production systems release more CO2 to the atmosphere than is taken up during growth of the biomass. Their schemes are: (1) Growth of algae in open ponds using a raceway configuration, with slow-moving paddle wheels to aerate and circulate the algae growth medium; (2) fertilizers are added as water is pumped in to or out of (for harvesting) the ponds; and (3) CO2 is bubbled into the ponds. The result of the analyses for a production site in California, for example, indicated that for producing 1.00 unit of energy, about 1.18 unit of energy is consumed; nutrients: 0.49 unit (about 0.2 unit for urea), CO2-derived: 0.35 unit, direct: 0.04 unit, and others (water, etc.): 0.29 unit. They pointed out that in addition to anticipated improvements in algal productivity (next-generation production), the uses of flue gas (from coal fired plants) and municipal wastewater (to reduce nutrient energy costs) could lead to a net-positive bioenergy production by microalgae in these systems.

3.3. Life-Cycle Analysis (LCA) of the Costs for Large-Scale Microalgal Production

A comparative LCA study of the potential environmental impact and economic viability of producing biodiesel from microalgae grown in large virtual ponds (4 km2) of coastal Australian land were made [43]. In terms of GHG (greenhouse gas) emissions, algae GHG (−27.6 to 18.2 (CO2-unit)) compare very favorably with canola (35.9) and ultra-low sulfur (ULS) diesel from oil (81.2). Costs are not so favorable, with algae ranging from 2.2 to 4.8 (cost-unit), compared with canola (4.2) and ULS diesel (3.8). The large footprint of algae cultivation is driven predominantly by upstream factors, such as the demands for CO2 and fertilizer. To reduce these factors, flue gas and, to a greater extent, municipal waste-water could be used to offset the economic and environmental burdens associated with algae, highlighting the need for a high production rate to make algal biodiesel economically attractive.

4. Our Scheme for Large-Scale Photobiological H2 Production by Mariculture-Raised Cyanobacteria

We briefly discuss several issues for achieving commercially viable large-scale photobiological H2 production by cyanobacteria. Photobiological H2 production is considered to be one of the better candidates for renewable energy production because H2 pollutes environment minimally both in production as well as in utilization stages, and is relatively easily storable and transportable.
We will first describe an outline of our conceptual scheme [44] for large-scale photobiological H2 production by mariculture-raised cyanobacteria. We will then discuss some of the key issues in greater detail. Our scheme is: (1) Production of H2 in large plastic bioreactors consisting of several layers of plastic film; (2) repeated harvesting of crude H2; (3) initial separation of H2 from O2 possibly by gas-selective permeability membranes on factory ships followed by further purification of H2 by pressure-swing adsorption (PSA); and (4) compression or transformation to a form suitable for transportation by ship and storage (Figure 3 and Figure 4).
Table 2. Expected sales of photobiologically produced H2.
Table 2. Expected sales of photobiologically produced H2.
Energy Conversion Efficiency (%)Produced H2 (kWh·m−2·yr−1)Energy Recovery (Ratio)Purified H2 (kWh·m−2·yr−1)H2 Total Sale (cents m−2·yr−1)
Selling Price (cents·kWh−1)
10203040
1150.34.54590135180
1150.57.575150225300
1150.710.5105210315420
2300.3990180270360
2300.515150300450600
2300.721210420630840
3450.39135270405540
3450.515225450675900
3450.7213156309451260
The ΔH of 1 kg crude oil (Oeq) is 41.9 MJ or 11.6 kWh (HHV, higher heating value: the product water is condensed liquid). The ΔH of 1 m3 (STP) H2 is 12.8 MJ, 3.56 kWh, or 0.30 kg·Oeq (Oil equivalent) and that of 1kg of H2 is 142 MJ, 39.4 kWh or 3.39 kg Oeq (HHV).
Assuming the total solar radiation of about 1500 kWh·m−2·yr−1 [10] and an energy conversion efficiency of 1%–3% (of total radiation), which will be discussed later, the energy produced as crude H2 is 15–45 kWh·m−2·yr−1 (Table 2). Assuming an energy recovery ratio (energy in purified H2/energy in crude H2) of 0.3–0.7, we calculated a total price for H2 of 10–40 ¢/kWh (cf. Section 1.3 for the price ranges of renewable fuels). Table 2 gives sales projections for photobiologically produced H2 and the energy conversion efficiency targets that will promote the adoption of photobiological renewable production.

4.1. Flexible Plastic Bioreactors Floating on the Surface of Sea Could Reduce Costs

Bioreactors for commercially viable algal biomass or liquid fuel production should be large (a total of a few km2 as a production unit) and inexpensive. Currently, open ponds with raceway configurations are the leading candidates for the first step of biomass production of algae. For H2 production, closed bioreactors are required in at least some part of the process. A variety of closed hard panel or tubular photobioreactors are described for laboratory or pilot-scale studies (e.g., [45,46]), but they are likely much more expensive than open ponds.
We have proposed flexible H2-barrier plastic bags floating on the calm sea or ocean surface (e.g., the calm belt about 30° north or south, such as the “mysterious Bermuda triangle” region) [17,44]. The culture medium is based on freshwater, and the bioreactors would spread over the sea surface because of the difference in density between the culture medium and the surrounding seawater. Salt lakes can also be used as the fields for cultivation. The size of the bags is flexible; for large-scale H2 production for example, 20 bags of 25 m × 200 m in surface area, could cover the surface of 1 km2. As proof of this concept, Kitashima et al. [47] demonstrated that transparent flexible H2-barrier plastic bags are usable for studies of photobiological H2 production by cyanobacteria in the laboratory. The H2 permeability (Pm) value of the transparent plastic bags ranged from 44 to 87 cm3·m−2·atm−1·day−1. H2-barrier bags for laboratory use (Wakhy bags, www.ab.auone-net.jp/~wakhylab) are now commercially available (GL Sciences, Tokyo. [email protected]).
The cost of the bioreactor was estimated as follows [44]. The bioreactor is composed of three layers of plastic bags (Figure 3), for a total of six layers (sunny side and shady side) of transparent plastic film. The innermost bag holds the cyanobacteria culture, the middle bag has very low permeability to H2, and the outermost bag serves to mechanically protect the inner bags. The thickness of each film is 0.08 mm, and 480 cm3 of plastic per·m2 of the bioreactor’s sunny side surface is required. Assuming an average plastic price of $2–$4 per kg (or liter), the material cost is 96–192 cents·per·m2 of bioreactor. The used plastic bags can be recycled many times to regenerate plastic films at about half the price of the new materials. The above assumptions result in the cost of the bioreactor being about 24–48 cents per·m2 of bioreactor surface per year, assuming a renewal cycle of every two years. The plastic films of 480 cm3 are assumed to be produced by consuming 360 mL of crude oil for processing that is equivalent to 3.92 kWh·per·m2 per year. The plastic bags can be recycled at an energy cost of 20% of the feedstocks (0.78 kWh). The amount of energy in feedstocks derived from fossil fuels can be further decreased because currently H2 generated from fossil fuels is used as a part of the feedstocks for plastic film production, and photobiologically-produced H2 can replace some part of it.

4.2. Cost-Effective Strategy for Achieving Adequate Cell Growth with Repeated Harvesting of H2 without Changing the Culture Medium

Under our proposed strategy, H2ase-less mutant cyanobacterial cells grow in large ordinary plastic bags containing CO2 (with its occasional replenishment) floating on the sea without mechanical agitation of the medium (Step 1, in Figure 3). The need for additional combined nitrogen for growth would be minimal and thus the cost of fertilizer would be much less as compared to systems using non-nitrogen-fixing microalgae. Cyanobacterial stock cultures are transferred to photobioreactors for H2 production (Step 2). The innermost bag (Figure 3) is filled with gas containing CO2 in Ar. In the H2 production stage, no mechanical agitation or bubbling are applied, as CO2 is recycled within the bag (absorbed during photosynthetic carbon assimilation in vegetative cells and released from heterocysts when saccharides are degraded as electron donors to N2ase (Figure 2)). The cyanobacterial cell waste can be recycled as fish feed [48].
Figure 3. Outline of H2 production by mariculture-raised cyanobacteria. Step 1: Cell growth in a transparent plastic bag floating on the sea surface. The bioreactor is filled with air containing CO2; Step 2: H2 production in a photobioreactor composed of three bags (at least one layer is a H2 gas barrier membrane) floating on the sea surface. The spent cells can be used as fish feed [48].
Figure 3. Outline of H2 production by mariculture-raised cyanobacteria. Step 1: Cell growth in a transparent plastic bag floating on the sea surface. The bioreactor is filled with air containing CO2; Step 2: H2 production in a photobioreactor composed of three bags (at least one layer is a H2 gas barrier membrane) floating on the sea surface. The spent cells can be used as fish feed [48].
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The proposed strategy can be modified in response to changes in production costs. For example, when the cost of Ar is high, N2ase mutants can be used [49]. Some of the mutants have high H2 production activity under N2-rich gas as compared to the parent strain activity under Ar gas, and also have extremely low N2-fixing activity. Examples of such mutants have been characterized; with the amino acid substitutions presumed to be located in the vicinity of the FeMo-cofactor of N2ase (e.g., Q193S and R284H) [49]. The N2ase activity of such mutants is not inhibited by the presence of high concentrations of N2 and thus the use of costly Ar could be avoided. However, these strains require combined nitrogen in the growth stage, and the advantages and disadvantages of using this type of mutant needs to be carefully assessed.

4.3. Initial Separation of crude H2 Followed by Further Purification by Pressure-Swing Adsorption (PSA) on Factory Ships

The H2 produced within the bag is allowed to accumulate for several weeks to a few months before “harvesting” the gas mixture (Figure 4). After removal of O2 from the harvested gas mixture, H2 is purified on factory ships by PSA (pressure-swing adsorption) for transportation to ports [44]. The separated Ar and CO2 are recycled back to the bioreactors, along with replenishment of H2O (substrate necessary for H2 production) to resume the next round of H2 production. The amount of H2O needed is relatively small, (0.8 kg H2O is required for 1 m3·H2, or 18 g for 22.4 L·H2). Some of the downstream technologies outlined in Figure 4 are still in the developmental stage, notably the initial separation of H2 from O2 in the gas mixtures. One of the candidate technologies involves the use of gas-selective membranes that allow the penetration of H2 at much higher rates than that of O2. For example, there is a report of a carbon molecular sieve membrane that allows permeation of H2 about 10–15 times faster than O2 (the gas permeability constant of 372–473 and 25–50 in gas permeability units for H2 and O2, respectively) [50]. We expect that there will be a concomitant development of these technologies if photobiological H2 production on the sea surface is adopted as one of the best options for large-scale renewable energy production (an example of “necessity is the mother of invention”).
Figure 4. Outline of photobiological H2 production by mariculture-raised cyanobacteria and delivery of purified H2 to end-users (possible scheme). The fully grown cells (Step 1, Figure 3) are transferred to the photobioreactor (Step 2, Figure 3), which is filled with Ar and CO2 (+ trace amount of N2, not shown) and allowed accumulation of the produced gases (H2 and O2). (A) Initial separation of O2 from the gas mixture; (B) Further purification of H2 by PSA (pressure-swing adsorption), and the removed CO2 and Ar are recycled to the bioreactor. H2O consumed for H2 production is replenished; (C) Purified H2 is processed for transportation to end-users (for details, see text).
Figure 4. Outline of photobiological H2 production by mariculture-raised cyanobacteria and delivery of purified H2 to end-users (possible scheme). The fully grown cells (Step 1, Figure 3) are transferred to the photobioreactor (Step 2, Figure 3), which is filled with Ar and CO2 (+ trace amount of N2, not shown) and allowed accumulation of the produced gases (H2 and O2). (A) Initial separation of O2 from the gas mixture; (B) Further purification of H2 by PSA (pressure-swing adsorption), and the removed CO2 and Ar are recycled to the bioreactor. H2O consumed for H2 production is replenished; (C) Purified H2 is processed for transportation to end-users (for details, see text).
Life 05 00997 g004
The purified H2 may be condensed (high pressure or liquefied) or chemically transformed (e.g., to NH3 which can subsequently be used as a fuel rather than fertilizer, or reversible hydrogenation of toluene (C7H8) to methyl cyclohexane (C7H14)) for transportation to end-users (Figure 4).

4.4. The Advantages of Sustained High H2 Production without Changing the Culture Medium

We would like to emphasize that one of the economic advantages of photobiological H2 production by cyanobacteria is that the culture medium can be used continuously. During the growth stage, cyanobacteria do not produce H2 and the input costs of labor, energy, nutrients, etc. are minimal. A major advantage that the N2ase-based photobiological H2 production by cyanobacteria systems have over the other types of algal biofuel production systems is that once established, cultures can produce H2 for a long time (several weeks) without changing the culture medium and with multiple rounds of gas harvesting [49,51,52] (Table 3), thus off-setting the initial costs of the cell growth phase. Several groups have reported the duration of active H2 production to be several weeks, and we expect that this could be further extended by carefully managing the culture conditions (Table 3). Attaining sustained high H2 production without changing the culture medium will mitigate costs of nutrients, a criticism raised by Clarens et al. [42] (see Section 3.2).
Table 3. Some records of duration (>2 day) of H2 production activity without changing the culture medium.
Table 3. Some records of duration (>2 day) of H2 production activity without changing the culture medium.
StrainsLight IntensityEfficiency (%)Light EnergyDuration of expt.GasRemarksRefs.
Anabaena cylindrica 6294.0 × 105 erg·cm−2·s−10.4% av.total rad.8 dAr/CO2 (99.7/0.3), gassing250 mL culture: about 0.6 L gas/h Cell density of 200–260 Klett units Periodic addition of 10−4 M·NH4Cl[53]
Anabaena cylindrica 62932 W·m−20.85% max.PAR6 dAr/CO2 (99.5/0.5), gassing0.875 L culture: 0.3–0.9 L gas/h[54]
Anabaena cylindrica 6296 W·m−20.35% av.PAR28 dAr/CO2 (99.5/0.5), gassing0.875 L culture: 0.3–0.9 L gas/h[54]
Mastigocladus laminosus NZ-86-m3.0 × 104 erg·cm−2·s−12.7% max.PAR2–3 dAr/N2/CO2 (98.5/1/0.5), gassing1.2 L culture[55]
Nostoc sp. PCC 7422 ΔHup deficient of Hup70 μmol photons m−2·s−13.7% av.PAR6 dAr/CO2 (9.5/5), (no gassing)6 mL batch culture[35]
Anabaena variabilis ATCC 2941332 W·m−20.96% av. 1.32% max.PAR8 dStage 1: Ar, gassing, Stage 2: air/CO2 (95/5), gassingH2 producing activity in stage 2[56]
Nostoc/Anabaena sp. PCC 7120ΔHup, site-directed N2ase variants, Q193S and R284H90–100 μmol photons·m−2·s−1not givenPAR21 dN2/CO2 (95/5), (no gassing with periodic gas replacement of every 3 or 4 days)Sustained, high-level production of H2 through 21 days[49]

5. Improvements Needed in the Energy Conversion Efficiency under Outdoor Conditions

If photobiological H2 production is to be developed as a source of large-scale renewable energy, improvements are needed in both the light energy conversion efficiency and in the rates of H2 production. The maximum theoretical energy conversion for N2ase-based photoautotrophic H2 production by cyanobacteria has yet to be precisely calculated. This is because N2ase requires a considerable amount of ATP and the energy conversion efficiency of photophosphorylation has yet to be conclusively determined. There is a lack of information on the structure and function of the membrane ATP synthase (H+-ATPase) that consumes the proton-motive force generated across membranes as the source of energy as predicted by the chemi-osmotic mechanism proposed by P. Mitchell [57,58]. Most likely, the H+/ATP ranges between 8/3 and 14/3 (for discussion, see [21,59,60]). By assuming an H+/ATP ratio of between 3 and 4, Sakurai and Masukawa [17] calculated the maximum energy conversion efficiency of between 16.3% and 13.9% for 550 nm light and between 7.3% and 6.3% for the total solar radiation, assuming cyanobacteria can use 45% (400–700 nm light, PAR: photosynthetically active radiation) of total radiation.
Of special significance is a report of a record high H2 production activity on a chlorophyll basis by cyanobacteria. The N2ase activity of the unicellular cyanobacterium Cyanothece sp. ATCC 51142 is regulated by circadian rhythms: photosynthesis in the light, and N2ase reaction in the dark. When the cells were grown in the presence of glycerol for 12 h under the light to accumulate photosynthetic products (the first stage), they showed high photobiological H2 activity on a chlorophyll (Chl) basis of 465 μmol mg Chl−1·h−1 when the illumination was continued for another 12 h (the second stage) [61]. This type of strain may be potentially useful if low cost organics are available, such as wastewater rich in useable organic compounds (e.g., from the food industry). However, as many of the heterocystous strains very poorly use organic compounds, this is currently not very promising for the improvement of H2 production by heterocystous strains.

5.1. Comparing Measured Values for Light Energy Conversion Efficiency of Photobiological H2 Production by Cyanobacteria to Our Tentative Target Values of 1.2%

Although values of 2.6%–3.7% of PAR in laboratory experiments were reported by several groups [35,55,62], the values drop to 0.2% or less in outdoor experiments lasting for more than two days [51,52,63,64] (daily maximum of 0.6%, Miyamoto [51]) (Table 4). For our proposed scheme, we believe that 1.2% (of total radiation) or 2.7% of PAR for outdoor conditions are reasonable targets for improved efficiency.
Table 4. Some records of light energy conversion efficiency and duration of the activity.
Table 4. Some records of light energy conversion efficiency and duration of the activity.
StrainsLight IntensityEfficiency (%)Light EnergyDuration of expt.GasRemarksRefs.
Mastigocladus laminosus NZ-86-m4.4 × 105 erg·cm−2·s−10.17% av.total rad.17–24 dAr/N2/CO2 (98.7/1.0/0.3), gassing1 L culture: 6.5 L·gas/h[52]
Anabaena cylindrica 629about 50–330 cal·cm−2·d−10.2% av. 0.6% max.total rad.36 dAr/N2/CO2 (balance/0.2–0.4/0.5), gassing0.8 L culture: 5.0 L·gas/h[51]
Anabaena variabilis PK84400 W·m−2 (sunny day) 100 W·m−2 (cloudy day)0.14% (sunny day) 0.33% (cloudy day) 18 dair/CO2 (98/2), gassingchemostat-type bioreactor, possibly V-type N2ase expressing conditions[65]
Anabaena variabilis PK84 deficient of the activities of both Hup and Hoxmax. 850 W·m−20.029%–0.094%total rad.40 dair/CO2 (98/2), gassingchemostat-type bioreactor, possibly V-type N2ase expressing conditions, June–July, London[64]
Anabaena sp. PCC 7120 AMC 414 deficient of Hupmax. 600 W·m−20.042% max.total rad.9 dair/CO2 (98/2), gassingchemostat-type bioreactor, August, London[63]

5.2. Some Potential Strategies to Achieve Higher Light Conversion Efficiencies

Many aspects of the H2 production and the related technologies are under development currently, making it challenging to estimate production costs. Nevertheless, such estimates are informative for both policy-makers and investors in R&D efforts. Sakurai et al. [44] presented a preliminary estimate of 26.4 ¢/kWh (assuming the price of plastics at $2 per kg) as a means to identify the needed R&D efforts to achieve efficient photobiological H2 production by cyanobacteria. The conditions were: (1) mariculture-raised cyanobacteria produce H2 at an energy conversion efficiency of 1.2% (18 kWh·m−2·yr−1) in plastic bioreactors floating on the sea surface (solar radiation 1500 kWh·m−2·yr−1); (2) the crude H2 is purified on factory ships and transported to final destination ports in storage tanks by container ships; and (3) the energy recovery (from production to the final commodity of H2) is 0.5. Although the tentatively estimated price above is more expensive than the currently levelized price of electricity, it is reasonably close to the prices in several countries with feed-in tariff schemes (see Section 1.3). The price of H2 can be further decreased with improvements in both light conversion efficiency and energy recovery, and by decreasing the processing costs with advancements in relevant technologies. Because photobiologically produced H2 contributes to the reduction of the greenhouse gas CO2 emissions, and because H2 fuel cells are expected to be more energy efficient than internal combustion engines, the R&D of photobiological renewable energy sources should be pursued in more earnest.
Amos [66] estimated the cost of H2 produced by Chlamydomonas to be 22.8 ¢/kWh when H2 is compressed and stored in high-pressure tanks for storage and transportation, and 7.2 ¢/kWh when direct connections to H2 pipelines are available. In certain locations, such as salt lakes, a pipeline could be used to transport gas products with reduction of the total cost of H2 photobiologically produced by cyanobacteria.

5.2.1. Selection of Strains with High N2ase Activity Outdoors Followed by Further Improvements via Genetic Engineering

Yoshino et al. [35] compared the photobiologically driven N2ase activity under laboratory conditions among 13 heterocystous strains maintained in academic centers, and selected Nostoc sp. PCC 7422. The uptake hydrogenase knocked out mutant (∆Hup) produced H2 at an energy conversion efficiency of 3.7% vs. PAR under laboratory conditions. Selection of strains with high N2ase activity under outdoor conditions with high light intensities followed by further targeted improvements via genetic engineering seems to one of the most promising strategies for achieving higher light conversion efficiencies.

5.2.2. Truncated Antenna Complexes

Light-saturation of photobiological activity is one of main reasons light conversion efficiencies are decreased under outdoor conditions as compared with the laboratory conditions for cyanobacteria. Many cyanobacterial strains have large antenna complexes containing pigments such as phycocyanin, which enable them to survive even under conditions of low light intensity such as in a dense culture or in sediment. In order for photobiological H2 production schemes of the culture as a whole to operate at optimum efficiency, large antenna size is a problem because cells near the surface absorb the most part of incident light and are unable to use it efficiently because of light saturation, while other cells beneath them receive only the residual low light. It is hypothesized that truncation of antenna size would help to alleviate excess absorption of sunlight and the ensuing wasteful dissipation of excitation energy, and to improve solar-to-product energy conversion efficiency and photosynthetic productivity in high-density mass cultivations. As proof of this concept, there are reports of truncated antenna cyanobacterial mutants showing higher rates of photosynthetic activity in culture over the wild-type strains [67].

5.2.3. Increase in Heterocyst Frequency

Under conditions of nitrogen deprivation, heterocystous cyanobacterial cells differentiate heterocysts at intervals of 10–20 vegetative cells, depending upon the strains. While heterocyst frequency may be optimized to support growth of the strains while fixing N2 under their ordinary natural habitats, the frequency can also be modified to increase H2 production because the cells do not grow in the H2 production stage and thus the supply of organic compounds for growth can be dispensed. Many genes involved in heterocyst differentiation have been reported and the mutants of several of these genes (via disruption, overexpression, and duplication of genes and point mutation) result in higher frequencies of heterocysts [25,26,68]. However, many of the mutants form multiple contiguous heterocysts and their N2ase activities measured by acetylene reduction do not exceed the wild-type activities. PatN is required for normal heterocyst patterning and has a role in the biased initiation of heterocyst differentiation. In Nostoc/Anabaena sp. PCC 7120, disruption of patN led to formation of multiple singular heterocysts. Although the patN mutant exhibited lower N2ase activity and diazotrophic growth rate compared with the wild-type [69], it will be interesting to see the effects of modification of heterocyst frequency on photobiological H2 production by other strains or under different experimental conditions.

5.2.4. Improvement of the Enzymatic Activity of N2ase

Other H2-producing enzymes, FeFe and NiFe H2ases, have high H2 production activity with a turnover rate of 6000–9000 and about 100 s−1, respectively, although the latter enzyme also has greater H2 uptake activity with a turnover rate of 450–600 s−1 [70]. In contrast, although N2ase has an advantage in catalyzing unidirectional production of H2, it has a very low turnover rate of about 6.4 s−1 [71,72]. The rate-limiting step in N2ase catalysis is the dissociation of the dinitrogenase reductase Fe protein (Complex 2) from the dinitrogenase MoFe protein (Complex 1). The dissociation occurs after ATP-coupled electron transfer between the two proteins. In the N2ase reaction, H2 is evolved initially when N2 binds to the enzyme. The slow protein dissociation is considered to contribute to maximizing N2 reduction by suppressing H2 evolution, futile to nitrogen fixation, at the midpoint of the whole reaction. It will be interesting to engineer N2ase, either MoFe-protein or Fe-protein, or both, by site-directed mutagenesis, to increase the turnover rate of H2 production by the enzyme.
When maintaining the N2ase-based reactions at high levels, cyanobacteria require high levels of amino acids to support the synthesis of the inefficient enzyme, and the increase in the specific catalytic activity will decrease the burden of protein synthesis.

5.2.5. Metabolic Engineering

As in other organisms, studies of genomes, transcriptomes, proteomes, and metabolomes are ongoing in cyanobacteria. The information from these studies will undoubtedly contribute to improving the overall activity of photobiological H2 production by cyanobacteria, as targeted improvements will be made [73]. For example, it will be interesting to pursue repression of the expression of glutamine synthetase in heterocysts. In normal cells, the enzyme is required for the massive export of fixed nitrogen from heterocyst to vegetative cells, and the gene expression level is greatly increased during the course of heterocyst differentiation [74]. In H2 producing cyanobacteria, however, massive glutamine transport is not necessary because the cells almost cease growing, and the investment of amino acids for the synthesis of proteins such as glutamine synthetase seems to be a waste of amino acid reserves.

6. Conclusions

Future Prospects for Large-Scale Photobiological H2 Production

In order for photobiologically produced H2 to make meaningful contributions to the mitigation of global warming caused by greenhouse gases, notably CO2, economical production of H2 is essential. Although many of the technologies required for the practical application of large-scale photobiological H2 production are in the development stages and the cost estimates of the produced H2 are preliminary due to various unpredictable factors, Sakurai et al. [44] presented a very preliminary estimate of 26.4 cents·kWh−1 of H2 produced on the sea surface using many presumptive assumptions, for example assuming the solar energy conversion efficiency of 1.2%. Currently, the maximum energy conversion efficiency of cyanobacterial H2 production under outdoor conditions is about 0.2%. There is an urgent need to demonstrate higher efficiencies to policy makers and developers in order to convince them of the potential benefits of photobiological H2 production by cyanobacteria. Increasing the solar energy conversion efficiency with improvements in technologies for purifying and transporting H2 will decrease the total cost. Public acceptance of renewable fuels very much depends upon the affordability of the price and will go a long way towards convincing consumers and government leaders to adopt technologies that will ultimately mitigate global climate change. Future cost estimates will be more accurate as the technologies in cyanobacterial H2 production and its related processes advance. We also expect that more refined cost estimates will allow for additional targeted improvements in the technologies, ultimately resulting in an overall cost reduction.
If we are able to produce H2 at 1.2% of total radiation (18 kWh·m−2·yr−1) on the sea surface and purified H2 is delivered to the end users with a final energy yield of 0.5, the net energy obtained is calculated to be 9 kWh·m−2·yr−1 or 32.4 × 106 J·m−2·yr−1 [44]. The current world fuel energy consumption is estimated to be 460 × 1018 J·yr−1 (Table 1, [3]). It follows that by using a surface of the sea equivalent to 1% of the global surface (1.36 × 106 km2, about 2.3 times the area of the island of Tasmania, or 3.1 times the area of the island of Great Britain), we will be able to replace 19% of the current world fossil fuel consumption.
In order to make a meaningful contribution to the mitigation of the hazards to the human population that are predicted to occur with global climate change, the promotion of R&D efforts for economical large-scale photobiological biofuel production and the advancements of biological and other needed technologies should be encouraged.

Acknowledgments

We thank Susan Carlson for critically reading the manuscript. This work was supported in part by grant-in aid for Scientific Research on Innovative Areas (No. 24107004) and Strategic Research Base Development Program for Private Universities from MEXT, Japan (to KI).

Conflicts of Interest

One of the authors (H.S.) is a stakeholder of Wakhy Laboratories.

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MDPI and ACS Style

Sakurai, H.; Masukawa, H.; Kitashima, M.; Inoue, K. How Close We Are to Achieving Commercially Viable Large-Scale Photobiological Hydrogen Production by Cyanobacteria: A Review of the Biological Aspects. Life 2015, 5, 997-1018. https://doi.org/10.3390/life5010997

AMA Style

Sakurai H, Masukawa H, Kitashima M, Inoue K. How Close We Are to Achieving Commercially Viable Large-Scale Photobiological Hydrogen Production by Cyanobacteria: A Review of the Biological Aspects. Life. 2015; 5(1):997-1018. https://doi.org/10.3390/life5010997

Chicago/Turabian Style

Sakurai, Hidehiro, Hajime Masukawa, Masaharu Kitashima, and Kazuhito Inoue. 2015. "How Close We Are to Achieving Commercially Viable Large-Scale Photobiological Hydrogen Production by Cyanobacteria: A Review of the Biological Aspects" Life 5, no. 1: 997-1018. https://doi.org/10.3390/life5010997

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