Physiologia Plantarum 131: 10–21. 2007 Copyright ª Physiologia Plantarum 2007, ISSN 0031-9317 REVIEW Photosynthetic biomass and H 2 production by green algae: from bioengineering to bioreactor scale-up Ben Hankamer a , Florian Lehr b , Jens Rupprecht a , Jan H. Mussgnug c , Clemens Posten b and Olaf Kruse c, * a Institute for Molecular Bioscience, University of Queensland, St Lucia Campus, Brisbane, Queensland 4072, Australia b Division of Bioprocess Engineering, Institute of Engineering in Life Sciences, University Karlsruhe, 76131 Karlsruhe, Germany c Department of Biology, Algae Biotech Group, University Bielefeld, 33501 Bielefeld, Germany Correspondence *Corresponding author, e-mail: [email protected]Received 22 December 2006; revised 12 March 2007 doi: 10.1111/j.1399-3054.2007.00924.x The development of clean borderless fuels is of vital importance to human and environmental health and global prosperity. Currently, fuels make up approximately 67% of the global energy market (total market ¼ 15 TW year 21 ) (Hoffert et al. 1998). In contrast, global electricity demand accounts for only 33% (Hoffert et al. 1998). Yet, despite the importance of fuels, almost all CO 2 free energy production systems under development are designed to drive electricity generation (e.g. clean-coal technology, nuclear, photovoltaic, wind, geothermal, wave and hydroelectric). In contrast, and indeed almost uniquely, biofuels also target the much larger fuel market and so in the future will play an increasingly important role in maintaining energy security (Lal 2005). Currently, the main biofuels that are at varying stages of development include bio-ethanol, liquid carbohydrates [e.g. biodiesel or biomass to liquid (BTL) products], biomethane and bio-H 2 . This review is focused on placing bio-H 2 production processes into the context of the current biofuels market and summarizing advances made both at the level of bioengineering and bioreactor design. Biofuel options Photosynthesis plays a central role in all biofuel production. It drives the first step in the conversion of light to chemical energy and is therefore ultimately responsible for the production of the feedstocks required for all biofuel synthesis (Fig. 1); protons and electrons (for bio-H 2 ), sugars and starch (for bio-ethanol), oils (for biodiesel) and biomass (for BTL products and biomethane). Consequently, any increase in photosynthetic efficiency (discussed below) will also enhance the competitiveness of biofuel production. Bio-ethanol Bio-ethanol is already well established as a fuel most notably in Brazil and the US (Goldemberg 2007). It is mainly produced from starch (derived from corn and wheat) and sugar (sugar cane) produced during photo- synthesis. To produce ethanol, starch is usually mixed with water and heated briefly, before adding enzymes to release sugars, if required. Yeast is subsequently added to ferment the sugars to ethanol, and the ethanol is then purified from the mixture by distillation and dehydration. Biodiesel Biodiesel is typically produced from the oils extracted from soybeans, rapeseed and oil palm (Jeong et al. 2004, Sanchez and Vasudevan 2006). However, recently low- input high-diversity mixtures of native grassland perennials (Tilman et al. 2006) and micro-algae (Xu et al. 2006) with Abbreviations – AOX, alternative oxidase; BTL, biomass to liquid; Cyt b 6 f, cytochrome b 6 f; H 2 ase, hydrogenase; LHC, light- harvesting antenna complex; PQ, plastoquinone; PS, photosystem. 10 Physiol. Plant. 131, 2007
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Physiologia Plantarum 131: 10–21. 2007 Copyright ª Physiologia Plantarum 2007, ISSN 0031-9317
REVIEW
Photosynthetic biomass and H2 production by green algae:from bioengineering to bioreactor scale-upBen Hankamera, Florian Lehrb, Jens Rupprechta, Jan H. Mussgnugc,Clemens Postenb and Olaf Krusec,*
aInstitute for Molecular Bioscience, University of Queensland, St Lucia Campus, Brisbane, Queensland 4072, AustraliabDivision of Bioprocess Engineering, Institute of Engineering in Life Sciences, University Karlsruhe, 76131 Karlsruhe, GermanycDepartment of Biology, Algae Biotech Group, University Bielefeld, 33501 Bielefeld, Germany
their high lipidand fattyacidcontent are also considered as
a suitable source. These are converted to biodiesel via
a transesterification reaction with methanol or ethanol in
the presence of a catalyst, to yield mono-alkyl esters and
glycerine, which is subsequently removed.
Biomass to liquid
BTL production (see: Kavalov and Peteves 2005) typically
begins with the grinding and drying of solid biomass (e.g.
wood, straw and corn) before forming it into pellets.
Through a low-temperature gasification process, these
biomass pellets are then converted into a gas (smouldering
gas) and solid fraction (charcoal). These are then trans-
formed into a synthetic gas in a second step. This gas is then
purified and liquefied via the ‘Fischer–Tropsch’reaction, inwhich carbonmonoxide (CO) and hydrogen (H) react and
form carbo-hydrogen chains. The product is a paraffin-like
liquid, which is then isomerised to increase its stability
before it is purified via distillation or ‘hydrotreatment’.
Biomethane (biogas)
Organic material like crop biomass or liquid manure canbe used to produce biogas via anaerobic digestion and
fermentation (Farquhar and Rovers 1973). Mixtures of
bacteria are used to hydrolyse and break down the
organic biopolymers (i.e. carbohydrates, lipids and
proteins) into monomers, which are then converted into
a methane-rich gas via fermentation (typically 50–75%
CH4). Carbon dioxide is the second main component
found in biogas (approximately 25–50%) and, like otherinterfering impurities, has to be removed before the
methane is used for electricity generation.
Bio-H2
Certain green algae and cyanobacteria (beyond the
scope of this review) have evolved the ability to harness
solar energy to extract protons and electrons from water
via the water-splitting reaction of PSII. In green algae,
these protons and electrons are then subsequently
recombined by a chloroplast hydrogenase (H2ase;
Happe and Naber 1993, Melis et al. 2000, Zhang et al.
2002) to form molecular H2, which is released from the
algal culture as a gas with a purity of up to 98% (Kruse
et al. 2005b).
Advantages of bio-H2 production
Given the choice of biofuels, it is worth briefly
summarizing the theoretical advantages of future bio-H2
fuel production systems, before describing recent devel-
opments of this biotechnology and the improvements
required to realize economic viability.
H2 – a promising future fuel
H2 has been identified as one of the most promising fuels
for the future (Abraham 2002, E.U. Commission 2002,
Koizumi 2002). The US, European Union and Japan have
already embarked on establishing H2 fuel stations, and in
parallel, car manufacturers have invested extensively in
the development of H2 fuel cell-powered cars.
Bio-H2: a sustainable alternative toconventional H2 production
Currently, the developing H2 economy is almost entirely
dependant upon the use of carbon-based non-renewable
resources [steam reformation of natural gas (approxi-mately 48%), petroleum refining (approximately 30%),
coal gasification (18%) and nuclear powered water
electrolysis (4%); Gregoire-Padro 2005]. Although these
resources are likely to drive the initial transition towards
a H2 economy, new, clean, sustainable and economic
ways of generating H2, such as solar powered bio-H2
production, will be required.
Fig. 1. The role of photosynthesis in biofuel production. Photosynthesis drives the first step in the conversion of light to chemical energy and is therefore
ultimately responsible for the production of the feedstocks required for all biofuel synthesis protons and electrons (for bio-H2), sugars and starch (for
bio-ethanol), oils (for biodiesel) and biomass (for BTL products and biomethane).
Physiol. Plant. 131, 2007 11
High-photon conversion efficiencies
The photon conversion efficiency (light to H2) cantheoretically be as high as approximately 10–16% (Kruse
et al. 2005a, Prince and Kheshgi 2005). Currently, how-
ever, such a high efficiency can only be approached for
transient periods, and this must be improved upon, for
economic viability to be achieved.
Carbon sequestration
Theoretically, solar powered bio-H2 production provides
a unique approach to CO2 sequester. During the aerobic
growth phase of the fuel production cycle, substantial
amounts of CO2 are absorbed and converted to biomass.
H2 is subsequently produced during the anaerobic phase,
with a large proportion of the sequestered carbon re-
maining in the form of biomass. In contrast, the com-
bustion of bio-ethanol, biodiesel, biomethane and BTLcarbohydrates release CO2, making these fuels at best
CO2 neutral, although the importance of this should not
be underestimated.
Fuel cells
Advances in fuel cell technology and the fact that the
combustion of H2 produces only H2O further increasesthe attractiveness of bio-H2.
Significance and innovation ofalgal biofuel systems
Another important factor to consider in the developing
biofuel area is whether to use conventional crops or algal
bioreactor systems. The acceptance of one approach over
the other will likely ultimately come down to a matter of
economics; however, algal bioreactors do offer a number
of important advantages.
Increased photon conversion efficiencies
Most plants have evolved genetic strategies to assemble
large light-harvesting antenna complexes (LHCI and II)
that give them a competitive advantage in terms of light
capture under low-light conditions. The downside of this
‘large antenna’ strategy is that at high light levels (e.g. up
to approximately 500 W m22), 80–95% of the absorbedphotons can be dissipated by these LHC proteins as
fluorescence and heat, via photoprotective mechanisms
(Polle et al. 2002). This occurs despite the fact that the
antenna is naturally, but only partially, downregulated in
size under these conditions (Escoubas et al. 1995, Melis
et al. 1999). Consequently, higher plants and wild-type
algae are not ideally suited for biofuel production.
Algal bioreactors can provide an engineering means to
regulate light levels to the culture not available to
conventional crop plants. The use of bioreactors therefore
opens up the possibility of using algal cell lineswith small
LHC antenna systems in which the amount of captured
light more closely matches the requirement of the cells athigh light levels. This in turn minimizes energy losses, as
fluorescence and heat. It also simultaneously increases
the photosynthetic efficiency of the cells at the illumi-
nated surface of the bioreactor and facilitates improved
light penetration into the algal culture. The latter allows
higher cell densities to be used to increase overall process
efficiency towards its theoretical maximum.
Reducing arable land use for biofuel production
A common concern related to biofuels is that as their
production capacities increase, so will the competition
with agriculture for arable land. In contrast, algal
bioreactors can be sited on non-arable land, eliminating
this competition and opening up new economic oppor-
tunities for arid regions.
Reducing H2O use in agriculture
Conventional crops used for biofuel production require
substantial amounts of fresh water. Because of the use of
closed bioreactors, considerable savings in the net water
use can be achieved.
Coupling clean fuel production to desalination
The use of marine algae has the theoretical potential to
couple bio-H2 production to desalination as the com-
bustion of hydrogen and oxygen extracted from seawater
yields fresh water. This approach requires stationary fuel
cells that use hydrogen and oxygen to feed electricity into
the national grid.
Advances in bioengineering of the solar bio-H2
process
As early as the 1930s, Gaffron and coworkers discovered
that under certain conditions unicellular green algae are
able to produce hydrogen during illumination (Gaffron
1939, Gaffron and Rubin 1942). Subsequently, the H2aseenzymes,which catalyse the recombination ofH1 and e2
to formmolecular H2, were shown to have a high specific
activity (approximately 1000 units mg protein21) (Florin
et al. 2001, Happe andNaber 1993). This level of specific
activity is approximately 100-fold higher than many of
otherH2ases (Adams 1990) and highlights the potential of
algal systems such as Chlamydomonas reinhardtii for
12 Physiol. Plant. 131, 2007
future solar poweredH2 production.However, in contrast
to cyanobacterial NiFe H2ases (Schutz et al. 2004,
Tamagnini et al. 2002), the algal H2ase was found to be
highly sensitive to O2 inhibition. In fact, it was not until
the groundbreaking work of Melis et al. (2000) that this
challenge was overcome through the cyclical depletionand repletion of liquidC. reinhardtii cultureswith sulphur
(Melis et al. 2000). The principle underlying this process
is that solar powered H2 production from water can be
divided into an aerobic and an anaerobic stage (1S stage:
PSII actively producing H1, e2 and O2, H2ases inactive;
and e2 to produceH2). This discovery formed the basis for
an expanding area of research focused on the engineeringof a more efficient bio-H2 production process. Melis and
coworkers, e.g. developed a sulphate transporter mutant
to restrict S supply for de novo synthesis of the D1 protein
of PSII (Melis andChen 2005). The rationale for thiswas to
engineer a mutant that could support low-level PSII
turnover during a continuous micro-oxic H2 production
process.
Recently, several micro-algae mutant strains related tobio-H2 production have been isolated in different
laboratories. These include strains with smaller LHC
antenna systems (Polle et al. 2003) leading to more
efficient light energy conversion, strains with low starch
content showing the direct correlation between H2
production and starch supply (Posewitz et al. 2004),
and a C. reinhardtii strain with high starch content and
a block in LHC state transitions resulting in a substantialincrease in H2 production capacity (Kruse et al. 2005b).
The latter strain was calculated to have a photon to H2
conversion efficiency of approximately 2% (from light to
H2) at 20 Wm22 in the presence of acetate, with a purity
of more than approximately 98%. The purity of the gas
was sufficient to power a fuel cell without further
purification (data not shown). Modified production
systems have since resulted in H2 production levels of850 ml H2 l
21.
The regulation and expression of the chloroplast H2ase
hydA isoforms are also an area of intense research, as is
their engineering to induce overexpression and a reduc-
tion of O2 sensitivity (M.C. Posewitz, A. Dubini, J.E.
Meuser, M.L. Ghirardi, in preparation).
To further improve the production efficiency, new
targets for bioengineering of the biophotolysis process inH2-producing micro-organisms need to be identified.
Consequently, many laboratories in the field of
microbial hydrogen production target this important
research area using systems biology approaches includ-
ing transcriptomics, proteomic andmetabolomic studies.
However, so far no data are available on analyses, which
directly refer to effects on H2 production pathways.
Nevertheless, in the near future, combined transcrip-
tomics, proteomics and metabolomic data will assist in
the in silico modelling of the complete H2 production
process and in targeting physiological bottlenecks for
bioengineering. These improvements will ultimately
interlink with parallel bioreactor development streams.
Efficiency considerations for scale-up
Before embarking upon scale-up, it is prudent to evaluatewhether bioengineering and bioreactor design streams
can at least in theory yield an economically viable solar
bio-H2 production process.
Current photon conversion efficiencies at20 W m22 illuminations
The culture flasks used in our laboratory have a surfacearea of 0.0142 m2 and are illuminated with 20 W m22
white light, resulting in an illumination level of 0.285 J
s21. The regular overall culturing time is 9 days (2 days
aerobic growth phase1 7 days anaerobic H2 production
phase) (Kruse et al. 2005b). During this time (777 600 s),
221 kJ radiation energy was transferred to the surface of
the culture, and in this experiment, 350 ml of pure
hydrogen gaswas produced on average (0.0156mol). Thecombustion reaction of hydrogen and oxygen has
a reaction enthalpy of 286 kJ mol21. The produced
hydrogen can therefore yield a maximum of 4.46 kJ of
energy, which corresponds to 2.0% of the transferred
irradiation energy.
Current photon conversion efficiencies atnatural light levels
In Europe, the average daytime irradiation levels are
approximately 230Wm22, which is more than a 10-fold
increase in illumination level over of that typically usedunder laboratory conditions (approximately 20 W m22)
(Kruse et al. 2005b). In addition, day and night cycles
reduce the illumination time to approximately 12 h
day21. Thus, a maximum of 9.94 � 103 kJ solar energy
can be absorbed per square metre per day at this
illumination level. If we assume that the photosynthetic
rate (and therefore the H2 production rate) correlates
linearly with the irradiation intensity up to natural lightlevels, this solar energy input could be converted into
0.695 mol H2 by an algal Stm6 culture with a photon
conversion efficiency of 2%. This corresponds to a H2
production rate of 1.39 g m22 day21. Melis et al. (1999)
showed a near linear increase in O2 production (a
measure of photosynthetic efficiency) of up to 1000mmol
m22 s21 illumination in high-light adapted Dunaliella
Physiol. Plant. 131, 2007 13
salina cells, which had a reduced antenna size. However,
it should be noted that a linear efficiency increase to
higher light levels (e.g., 2700mmolm22 s21) is only likely
to be approached using LHCII-deficient mutants, which
have already been constructed (Polle et al. 2003) but have
not yet been introduced into high-H2-producing strains.
Plant size at current efficiency levels
Based on the considerations above, a production plant
with a culture surface area of 1000 m2 (array of plate
reactors) could, e.g., yield 1.39 kg H2 day21, which is
equivalent to 15 568 l at standard conditions. If it is
possible to enhance the photon conversion efficiency to5% by means of genetic engineering and process
optimization, this would result in a hydrogen production
rate of 3.48 g m22 day21. Thus, the plant would produce
38 976 l H2 day21. If the upper photon conversion
efficiency limit of 10.6% could be reached, the pro-
duction rate could be as high as 7.37 g m22 day21,
equivalent to 82 523 l H2 day21.
Further production improvements
It should be taken into account that these calculations are
based on an irradiation intensity of 230Wm22. For other
geographical areas with higher irradiation levels (e.g.
Australia with approximately 545 W m22), the pro-
duction rates could potentially be higher if the light
saturation point is not reached and if no other negativereactions as result of high light levels occur (Barber and
Andersson 1992). In addition, the use of small antenna
mutants, which eliminate much of the 80–95% of energy
lost through fluorescence in the normal system, could
result in major yield improvements. This is because of
both improved photocapture efficiencies as well as light
penetration properties. These in turn will also allow
higher cell densities to be used in the bioreactor,potentially facilitating further improvements.
Bioreactor design
The two-phase process
Currently, bio-H2 frommicro-algae is produced in a two-
phase process, in which photosynthetic growth and H2
production are physically separated (Fig. 2). The advan-
tage of this approach is that it separates O2 (Fig. 2A) and
H2 production (Fig. 2B), preventing O2 inhibition of the
H2ase during the H2 production phase (Happe et al.
2002, Melis et al. 2000). An additional advantage is that
temporal separation is a useful way of improving H2
purity.
Light energy is essential for the process because it
drives photosynthetic cell growth as well as the hydrogen
production by photolytic water splitting. Compared with
fermentative hydrogen production by non-photosyn-
thetic bacteria, the biophotolytic process can in theory
be far more efficient (Rupprecht et al. 2006). This isbecause here light energy is directly coupled to hydrogen
production (via H2ase enzymes), whereas fermentative
bacteria have to metabolize fixed carbon sources.
In the first phase of this two-phase bio-H2 process
(Fig. 2A), the cells are grown aerobically to accumulate
biomass. To induce H2 production in the second phase,
the cells are transferred into a sulphur-depleted medium.
Alternatively, the sulphur concentration of the initialgrowthmedium can be adjusted appropriately for a given
cell density (Kosourov et al. 2002). Sulphur is needed for
amino acid synthesis, and so in sulphur-depleted
medium, protein synthesis cannot function properly and
degraded proteins cannot be replaced. This particularly
affects proteins with high turnover rates, such as the
D1 protein, a key component of PSII (Ohad et al. 1984).
Thus, in the absence of sulphur, the water-splitting reac-tion of PSII (2 H2O / 2 H2 1 O2) can therefore not be
maintained as the damaged D1 proteins cannot be
replaced. Consequently, O2 production decreases over
time. Simultaneously, O2 consumption via oxidative
respiration, alternative oxidase (AOX) activity in the
mitochondria as well as chlororespiration result in an
overall reduction in cellular O2 concentration in the
illuminated culture, and this ultimately leads to anaero-biosis and the onset (Fig. 2B) of H2 production after
approximately 24 h (Melis et al. 2000).
The efficiency of the two-phase process is dependant
on factors such as light level and distribution, pH,
temperature, media composition and substrate feeding
(Fedorov et al. 2005, Kosourov et al. 2002), all of which
are directly affected by the design of the bioreactor.
As an advancement on this theme, a continuoushydrogen photoproduction process was reported by
Fedorov et al. (2005). In this system, two stirred photo-
bioreactorswerebuilt to operate in parallel in a chemostat
mode, thereby separating the aerobic biomass produc-
tion from anaerobic H2 production phases.
The problem with using stirred tank reactors for
establishing such a continuous bioprocess is that they
are characterized by a high degree of back-mixing, re-sulting in a residence-time distribution of the cells in the
reactor. This in turn leads to a statistical age distribution
and thus a lowering of productivity. For biomass pro-
duction, back-mixing effects are favourable, but for H2
production, plug flow reactors are likely more suitable. In
such systems, the residence time can be adjusted more
precisely bymeans of reactor lengths andvolumetric flow
14 Physiol. Plant. 131, 2007
rate, and this in turn allows the cultures to bemaintained in
the optimal log-phase range for longer. Also, othernegative
aspects of stirred tank reactors related to photobiotechnol-
ogy, like high-light gradients, can be minimized usingtubular or plate systems (Janssen et al. 2003).
Further advantages of the two-stage system are that
semisterile photobioreactors can be used for the H2
production phase, thereby lowering the overall pro-
duction costs, particularly as the purity of the produced
H2 gas is already high enough for direct electricity pro-
duction in fuel cells (Kruse et al. 2005b). By eliminating
the need for sterilization, the material requirements are
much lower (e.g. reduced temperature and pressure
stability). This in turn extends the range of materials that
can be used into a lower cost bracket, and the reactor
design can simultaneously be simplified.
One-phase versus two-phase systems
The two-phase system (i.e. aerobic plus anaerobic stage)
does, however, carry a penalty in terms of the maximum
attainable photon conversion efficiency. This is because
three photons are required to transfer one e2 from H2O
to H2ase (photon 1: extracts e2 from H2O; photon
Fig. 2. Photosynthetic H1/e2 flow in C. reinhardtii under aerobic and anaerobic conditions in WT and H2 high-production mutant Stm6. (A) Under
aerobic conditions, e2 derived from the water-splitting reaction of PSII are passed along the photosynthetic e2 transport chain (solid black arrows) via
plastoquinone (PQ), cytochrome b6f (Cyt b6f), PSI and ferrodoxin (Fd). H1 released into the thylakoid lumen by PSII and the PQ/PQH2 cycle (H1 flow
indicated by solid grey arrows), generate a H1 gradient, which drives ATP production via ATP synthase. Dashed lines indicate H1 and e2 transfer pathways
inhibited in Stm6. (B) Under anaerobic conditions, H1/e2 stored in starch and NADPH are fed to H2ase for H2 production. In Stm6, cyclic e2 transport
(dashed line connecting Fd and Cyt b6f) is inhibited. The addition of an uncoupler (i.e. carbonylcyanide-m-chlorophenylhydrazone) results in an increased
H1 supply to the H2ase (HydA), resulting in an 9� increased rate of H2 production (Kruse et al. 2005b). This suggests that with cyclic electron transport
inhibited in Stm6, e2 supply has been increased to such an extent that H1 supply has become limiting.
Physiol. Plant. 131, 2007 15
2: transports the e2 through PSI, allowing it to form
NADPH and starch; photon 3: is required to transfer the
e2 from starch through PSI to H2ase).
In contrast, a one-step direct H2 production process (in
which PSII turnover and HydA-mediated H2 production
occur simultaneously under micro-oxic conditions) onlyrequires two photons (photon 1: extracts e2 from H2O;
photon 2: transports the e2 through PSI to the H2ase).
Consequently, this system could in theory yield a 33%
increase in efficiency. To achieve this, however, either
O2 insensitivity HydA mutants will be needed to be
developed (Ghirardi et al. 2006) or the rate of O2 con-
sumption must be higher or equal to the rate of O2
production, so that micro-oxic conditions that do notinhibit H2ase are maintained. Stm6, with its high O2
consumption capacity, is well suited for this purpose
(Kruse et al. 2005b) as it has an increased AOX activity,
which assists in the rapid activation of the H2ase.
Furthermore, it induced H2 production approximately
4 h earlier than in the wild-type (WT) with higher
subsequent production rates.
In a parallel approach, it has been shown that PSIIactivity can be maintained at low levels when very low
amounts of sulphur are added to the culture medium
(Kosourov et al. 2002). Using mutants with a high O2
consumption capacity under such conditionsmay indeed
offer further improvements as the rate of PSII-drivenwater
splitting could continue at higher levels and so support
a faster rate of substrate supply without inducing O2
inhibition. Such an approach will likely be necessary as
part of a strategy to achieve photon conversion efficiency
from light to H2 of 10%.
Light levels and distribution
Perhaps one of themost important issues to investigate on
the path towards commercial H2 production is the
linearity of the relationship between light intensity and
the hydrogen production rate. Such measurements
require specially designed photobioreactors in which
light gradients are minimized and light intensity canbe controlled over a wide range. A photobioreactor has
been developed (personal communication) especially for
kinetic studies under highly controlled light levels
(Csogor et al. 2001). The reactor is a 3-l stainless steel
stirred draft tube reactor (Fig. 3), which combines the
advantages of a stirred reactor (homogeneity) and a plate
reactor (short-light path length). Currently, this reactor
model is being modified to attain light intensities up toan approximately 1300 mmol m22 s21. A new internal
light system with high-performance light-emitting diodes
arranged on a cylindrical double-sided printed circuit
board has been installed inside the draft tube (Fig. 3B).
The electrical circuits of both sides can be controlled
Fig. 3. (A) Scheme of the 3-l stirred draft tube reactor system, developed for kinetic studies under highly controlled light levels. A propeller stirrer is used
to homogenize the biosuspension, which results in an axial liquid flow, streaming downwards inside the draft tube and upwards in the gap between the
vessel wall and the outside of the tube. The reactor can be operated in turbidostat mode. (B) Design drawing of the draft tube with internal light-emitting
diode system, which is used in the photobioreactor, to generate an almost homogenous light distribution.
16 Physiol. Plant. 131, 2007
separately, so that a homogenous light distribution inside
the reactor can be realized. Such systems are required to
measure the general kinetics of hydrogen production at
natural light levels and under conditions of light fluctua-
tions (e.g. light–dark cycles).
Light quality and distribution within the bioreactoritself is also of fundamental importance, as all photo-
trophic micro-organisms need light as an energy source.
Because of the absorption and shading effects, the light
intensity drops exponentially from the surface to the
centre of the reactor. This results in an uneven light
distribution inside the reactor. Amajor design criterion for
photobioreactors is therefore to achieve a high surface to
volume ratio, which minimizes light gradients. For thisreason, tank reactors have generally been considered less
suitable for photobiotechnological applications, as mix-
ing results in individual cells being exposed to constantly
changing light regimes, which are likely to reduce
production efficiency.
Reactor costs also significantly affect the price of the
produced hydrogen. It is therefore important to simplify
the design and minimize the cost towards <V10 m22
(Amos 2004). Newly developed plastic compounds, e.g.,
offer a great variety of alternative construction materials
for photobioreactors and are able to replace costly glass
and steel. Special properties that must be taken into
account include strength, durability, spectral properties
and its diffusion coefficient for hydrogen.
Systems currently under consideration include thin-
layer bioreactor systems (Pulz 2001), plate reactors,biocoil technology (Borowitzka 1999) and a range of
related immobilized systems (Laurinavichene et al. 2006,
Rupprecht et al. 2006).
Of the above, plate reactors offer themost homogenous
light distribution as a result of their high surface to volume
ratio. Indeed, an almost homogenous light distribution
can be realized byminimizing the plate depth. This has to
be accompanied by an increase of the cell density tominimize photon loss. Thin-layer bioreactor systems take
both of these considerations into account by using the
natural adhesion power between two hydrophilic materi-
als (i.e. foils, plastics and glass) to produce a thin liquid
film between them. Culture growth occurs to high density
within this film or on its surface (immobilized micro-
algae). Suspension and immobilization processes using
biocompatible nano-adhesive surfaces are anotherrelated alternative.
Minimizing energy use
To increase the energy efficiency of the bioreactor, the
energy required to pump or stir the culture must be
minimized. Energy efficiency can be increased by using
the H2 produced as a pneumatic energy source to mix the
culture. If this energy input is not sufficient to reach the
necessary mixing quality, a split stream of the produced
gas can be recycled to improve the mixing properties.
Using the H2-rich process, gas may in fact have the
additional benefit of maintaining anaerobic conditions.One such quasicontinuous hydrogen production system
with minimized energy input can be realized by establish-
ing an array of plate reactors. Each single plate reactor runs
through a two-stage process (aerobic growth/recovery
phase and anaerobic H2 production phase). The quasicon-
tinuous hydrogen production is achieved by a controlled
reversal between the single plates, similar to a quasicontin-
uous chromatography system consisting of several col-umns. By using immobilized cells, the system’s quality can
be further enhanced. Compared with the continuous
process described by Fedorov et al. (2005), such a set-up
potentially has three three theoretical advantages:
(1) optimal reactor geometries for light capture,
(2) enhanced production efficiencies based on uni-
form cell ageing profiles and
(3) modular scale-up.
Converting biomass waste stream to fuels
Biomass is one of the main byproducts of the solar bio-H2
process. There are several ways of producing biogases
from biomass. These include anaerobic fermentation,
gasification or pyrolysis (Demirbas and Balat 2006, Li
et al. 2004, Matsumura et al. 2005, Shizas and Bagley2005). The produced biogas can itself be used for H2
production through steam reforming. There are also
approaches to convert high-hydrous biomass directly
into hydrogen through hydrothermal gasification by using
supercritical water (Matsumura et al. 2005). Based on the
DWof the residual algal biomass after a laboratory-based
H2 production run and reported H2 production yields
frombiomass gasification,we estimate that gasification ofthe biomass waste stream could yield a further 5%
increase in total H2 production (unpublished results).
However, given the advance of BTL technology, new
avenues of waste to fuel conversion can be explored.
Nutrient optimization
Nutrient optimization has also proven to be a criticalcomponent for efficient biomass and bio-H2 production.
For example, within the first day of S-deprivation (and
nutrient deprivation in general) C. reinhardtii reacts by
accumulating large amounts of starch in the chloroplast,
while photosynthesis and subsequent Calvin cycle
reactions appear to remain active (Grossman 2000). The
accumulation of starch is an important precondition for
Physiol. Plant. 131, 2007 17
indirect H2 (i.e. the three-photon process described
above). This correlation was demonstrated by the low
H2 production phenotype of an isoamylase knockout
mutant (Posewitz et al. 2004), by the high H2 production
phenotype of Stm6, which is enriched in starch (Kruse et
al. 2005b) and through PSII inhibition experiments duringthe S-deprivation process (Fouchard et al. 2005).
Acetate is another critical component of the mixotro-
phic Tris acetate phosphate (TAP)medium as it is reported
to promote starch synthesis, thereby drastically extending
the period of starch availability for H2 production
(Fouchard et al. 2005). Consequently, acetate promotes
the cellular H2 production capacity.
The TAP medium typically used for H2 productionexperiments with C. reinhardtii was developed in 1965
(Gorman and Levine 1965). Early attempts of improve-
ment concentrated on the effect of the nitrogen sources on
H2 production. For example, it was demonstrated that
NH41 as the sole nitrogen source had an enhancing effect
onH2production (Aparicio et al. 1985). Recently, a 150%
increase in the hydrogen production ratewas observed by
modifying the standard TAP medium to NH41, 9.20 mM;
PO432, 2.09 mM and pH 7.00.
The influence of the extracellular pH onH2 production
has also been investigated at different stages of the
production cycle (Kosourov et al. 2003). Overall, the op-
timal pH for WT cultures has been reported to be pH 7.7.
Raising the pH to 8.2 delayed the onset of H2 production
by almost 100 h compared with the onset at pH 6.5.
Furthermore, towards the later part of the H2 productionphase, the rate dropped more markedly at pH values
below 6.5 and above 8.2 (Kosourov et al. 2003).
Another point of optimization is the reduction ofmedia
costs. In the case of TAP medium, the Tris buffer
component accounts for approximately 70% of the total
cost. We have already shown that Tris concentrations can
be reduced by 50%, with clear implications for reduced
production costs (unpublished results).As discussed earlier, acetate is important for the
establishment of anaerobiosis and is reported to be
relatively expensive, based on current market prices
(Fouchard et al. 2005). However, its concentration can be
lowered. Furthermore, acetate is a general waste product
from many biotechnological bacterial processes and
indeedwaste water treatment. This opens up the potential
for the linkage to pretreated waste streams.
Medium exchange
Medium exchange (e.g. S1/S2) is also a costly process,
and centrifugation of cells for this purpose is impractical
for scale-up. In this context, it is of note that Laurina-
vichene et al. (2002) successfully demonstrated a dilution
process that takes into consideration the consumption of
sulphur through cell amplification. This procedure also
reduces the risk of contamination.
Water recycling
An additional advantage of photobiotechnological
hydrogen production, compared with bio-ethanol and
biodiesel production, is that the subsequent combustion
of H2 andO2, e.g., by an on-site fuel-cell system linked to
the electricity grid, would not only recycle water but also
purify it as the combustion of H2 and O2 is pure water.
This is also an important advantage compared with the
cultivation of crops as energy feedstocks, where up to1000 l of water are reported to be required per kg
biodiesel produced.
Down stream gas purification
Another important issue for optimization is the gas purity
because most fuel-cell types need highly pure hydrogen.
In contrast to other hydrogen production processes likesteam gas reforming of fossil fuels, there are no critical
sulphur or carbon monoxide impurities (which act as
catalyst poison in fuel cells) in the gas produced by algae,
which consists mainly of hydrogen (approximately 98%)
and smaller amounts of N2, O2 and CO2 during the
hydrogen production process. Such high purities are
necessary even in continuous large-scale processes to
avoid expensive gas purification steps like pressure swingadsorption (Iyuke et al. 2000, Sircar and Golden 2000) or
membrane-basedmethods (Adhikari and Fernando 2006,
Hagg and Quinn 2006, Nenoff et al. 2006).
Conclusion
This review has outlined the importance of H2 and in
particular sustainably produced bio-H2 as part a future
clean energy mix and highlighted a selection of many
developments at the level of bioengineering a bioreactordesign on theway to developing economically viable bio-
H2 production systems. Substantial progress has been
made in facilitating continuous bio-H2 production and
enhancing production efficiencies through the engineer-
ing of light-harvesting antenna systems, optimizing
photon conversion efficiencies (direct vs. indirect bio-
H2 production), substrate supply to the H2ase, reducing
oxygen sensitivity of the system and many adaptations tobioreactor design. With H2-powered cars now being
developed bymost of the large car manufacturers and the
number of H2 fuel stations increasing, there is a clear
demand to improve clean and cost-effective bio-H2
production systems. This will likely require that H2
18 Physiol. Plant. 131, 2007
production levels will have to be increased from their
current level of approximately 2% at 20 W m22 illu-
mination (e.g. Kruse et al. 2005b) towards approximately
7–10% at normal daylight levels. The fact that reduced
antenna mutants are already reported to have photosyn-
thetic efficiencies (to O2) of approximately 10% (Melis etal. 1999) supports the view that economically viable H2
production is indeed a realizable goal. The value of
reaching this goal was clearly stated by Sir Nicholas Stern
in his recent report on the Economics of Climate Change
(Stern 2007): ‘markets for low-carbon energy products are
likely to be worth at least $500 billion per year by 2050,
and perhaps much more. Individual companies and
countries should position themselves to take advantage ofthese opportunities’.
References
Abraham S (2002) Towards a More Secure and Cleaner
Energy Future for America: National Hydrogen Energy