Introduction of closed cycle gas turbines with
their capability of retaining combustion generated CO2 can offer a
valuable contribution to the
Over the last years the authors have presented a design solution for this oxy-fuel CO2
retaining gas turbine system which can by acceptance of international gas
turbine industry be put into operation within a few years. The authors believe, that this system is equal in thermodynamic
performance to any other proposal in the field of Carbon Capture and Storage
(CCS) and is superior in applying gas turbine experience and research
accumulated to our day.

History and Continuous Development
The basic principle of the so-called Graz Cycle has been developed by H.
Jericha and presented at the CIMAC conference in
ASME Turbo Expo 2004,
At the ASME IGTI conference 2004 in
ASME Turbo Expo
2005, Reno-Tahoe, USA [15]:
Due to this favorable economic data the Norwegian oil and gas company Statoil ASA
initiated a cooperation in order to conduct a
feasibility study together with a major gas turbine manufacturer with the goal
of a technical and economic evaluation. In [15] the
basic thermodynamic assumptions for component losses and efficiencies agreed
with Statoil for a 400 MW Graz Cycle plant are shown
and the resulting power cycle for natural gas firing is presented. Its net
efficiency of 52.6 % is below the first simulations, but is still above most
alternative CO2 capture technologies.
ASME Turbo Expo 2006,
In order to avoid the difficulties of condensation of water
out of a mixture of steam and incondensable gases at very low pressures, at the
ASME 2006 [17] a modified cycle configuration was
presented with condensation in the range of 1 bar. It allows a separate
bottoming steam cycle with reasonably high pressures and efficiencies, so that a high net cycle efficiency above 53 % can be expected.
A design concept for a Graz Cycle plant of 400 MW net output
is presented with two shafts. A fast running compression shaft is driven by the
compressor turbine HTTC, whereas the power shaft comprises the power turbine
HPT and the LPST.
ASME
In
2008 the Graz Cycle turbomachinery were changed to higher pressure and
temperatures. A new pre-compressor for the working fluid allows to maintain the volume flow for the succeeding compressors,
so that they remain nearly identical. The new turbomachinery result in a Graz
Cycle power plant of 600 MW power output. Due to the higher cycle parameters of
50 bar and 1500°C, a net cycle efficiency above 55 %
can be expected.
ASME
Turbo Expo 2010,
In 2010
the Graz Cycle was adopted for the use of syngas from coal gasification. Syngas containing carbon monoxide, carbon dioxide
and hydrogen is fed to the Graz Cycle combustor,
the carbon dioxide separation takes place by condensation. Heat of the
gasification process is used in the Graz Cycle plant. The oxy-fuel technology
of the Graz Cycle is then compared with a pre-combustion plant, where the
carbon monoxide is converted to carbon dioxide by shift reaction and separation
of the carbon dioxide from the syngas
is done by chemical absorption. The comparison shows a higher efficiency for the
Graz Cycle plant.
ASME Turbo Expo 2011, Vancouver, Canada [24]:
In order to In
order to facilitate construction of a demonstration plant the performance of a
near-term Graz Cycle process design based on modest cycle data and available
turbomachinery components using a simplified flow scheme is presented at the
2011 ASME conference. Two near-term Graz Cycle plants are presented based on
basic and advanced operating conditions of the proposed commercially available
turbine. The predicted optimum net efficiency achieved is 23.2 % (HHV).
A near-term zero-emission power plant can only be
commercially attractive if it will be deployed in a niche market. Therefore an
economic analysis commensurate with an early pre-FEED conceptual study is
carried out for the U.S. Gulf Coast where revenue from multiple product streams
that could include power, steam, CO2 and water, as well as argon and
(potentially) nitrogen from the ASU is provided. The economic analysis suggests
that a capital investment of $94 million can secure construction of a
13.2 MWe
zero emission oxyfuel power
plant and yield a 14.5% (unlevered) return on capital
invested.
Economic Analysis
In an economical analysis the Graz Cycle power plant is compared with a
reference plant. The assumptions for capital costs, fuel costs and O&M
costs as well as the economical parameters are listed in [17]. The resulting mitigation costs are in the range
of 20 – 30 $/ton CO2 avoided depending on the costs of the air
separation unit (ASU) and thus are below a threshold value of 30 $/ton CO2
(assumed for future CO2 emission trading). This makes the Graz Cycle
an economically interesting solution for future CO2 capture.

CO2 mitigation costs vs. capital costs
Basic cycle configuration [15]
Basically the Graz Cycle consists of a high temperature Brayton cycle (compressors C1 and C2, combustion
chamber and High Temperature Turbine HTT) and a low temperature Rankine cycle (Low Pressure Turbine LPT, condenser,
Heat Recovery Steam Generator HRSG and High Pressure Turbine HPT).
The fuel (natural gas) together with the nearly stoichiometric
mass flow of oxygen is fed to the combustion chamber, which is operated at a
pressure of 40 bar. Steam as well as a CO2/
H2O mixture is supplied to cool the burners and the liner.
A mixture of about 74 % steam, 25.3 % CO2, 0.5 % O2
and 0.2 % N2 (mass fractions) leaves the combustion chamber at a
mean temperature of 1400 C. The fluid is expanded to a pressure of 1.05
bar and 579 C in the HTT. Cooling is performed with steam coming from the HPT,
increasing the steam content to 77 % at the HTT exit. The hot exhaust
gas is cooled in the following HRSG to vaporize and superheat steam for the
HPT. But after the HRSG only 45 % of the cycle mass flow are
further expanded in the LPT. The LPT exit and thus condenser pressure is 0.041
bar for a cooling water temperature of 8°C.

Principle flow scheme of basic S-Graz Cycle power plant
Gaseous and liquid phase are separated in the condenser. From there on
the gaseous mass flow, which contains the combustion CO2 and half of
the combustion water, is compressed to atmosphere with intercooling
and extraction of condensed water. CO2 is supplied for further
use or storage.
After segregating the remaining combustion H2O, the water
from the condenser is preheated, vaporized and superheated in the HRSG. The
steam is then delivered to the HPT at 180 bar and 549 C. After the expansion it
is used to cool the burners and the HTT stages.
The major part of the cycle medium, which is separated after the HRSG,
is compressed using an intercooled compressor and fed
to the combustion chamber with a maximum temperature of 600 C.
The cycle arrangement of the
Modified cycle configuration with working fluid condensation
at 1 bar [17]
Recent research shows that difficulties in condensation arise in the
formation of water films on the cooling tubes and in concentration of CO2
forming a heat transfer hindering layer so that only a low heat transfer
coefficient in condensation will be achieved. This results in excessively large
condenser heat transfer surface and related high costs. Therefore it was
suggested to condense this mass flow at atmosphere, separate the combustion CO2
and re-vaporize the water at a reduced pressure level using the condensation
heat. The pure steam is then fed to a Low Pressure Steam Turbine LPST, where it
can be expanded to a condenser pressure lower than that for the working fluid
mixture.
In the novel configuration the process is now split into the
high-temperature cycle and a separate low temperature condensation process as
shown in the following simplified scheme. The high temperature part consists of
HTT, HRSG, C1/C2 compressors and HPT. Condensation of the working fluid in the
1 bar range is proposed in order to avoid the problems of a working fluid
condenser at vacuum conditions as described above. The heat content in the flow
segregated after the HRSG for condensation is still quite high so
re-evaporation and expansion in a bottoming cycle is mandatory.

Principle
flow scheme of modified
This bottoming cycle operates by pure steam with extensively cleaned
feed water and thus allows together with the very low cooling water
temperatures of northern
For proper re-evaporation two sections of working fluid condensations
are provided, each following a compressor stage with reasonable increase of
flow pressure resulting in a higher partial condensation pressure of the water
content. At the first pressure level of 1.27 bar about
63 % of the water content can be segregated, so that the power demand of the
second compression stage is considerably reduced. It compresses up to 1.95 bar, which allows the segregation of further 25 % of the
contained water. Further cooling of the working fluid, also for water
preheating, leads to the separation of additional 11 %, so that the water
content of the CO2 stream supplied at 1.9 bar
for further compression is below 1 %. After segregation of the water stemming
from the combustion process, the water flow is degassed in the deaerator with steam extracted after the HPT and fed to the
HRSG for vaporization and superheating.
This two-step pre-compressed condensation counteracts the effect of
sinking H2O partial pressure due to condensed water extraction from
working fluid and thus allows a reasonably high constant re-evaporation
pressure of 0.75 bar for the bottoming steam cycle.
[2] Jericha, H., Fesharaki, M., 1995, "The Graz
Cycle 1500 C Max Temperature-CO2 Capture with CH4-O2 Firing", ASME
paper 95-CTP-79, ASME Cogen-Turbo Power Conference,
[3] Lukasser, A., 1997,
"Graz Cycle, eine Innovation zur
CO2 Rückhaltung", Master thesis, Graz University
of Technology.
[4] Tabesh, H., 1997,
"CH4-Graz-Cycle: Optimierung und Auslegung der Wärmetauscher",
Master thesis, Graz University of Technology.
[5] Jericha, H., Fesharaki, M., Lukasser, A., Tabesh,
H., 1998, "Graz Cycle – eine
Innovation zur CO2-Minderung", BWK Bd. 50
(1998), Nr. 10, Seiten 30-34.
[6] Jericha, H., Lukasser, A., Gatterbauer, W., 2000, "Der Graz Cycle
für Industriekraftwerke gefeuert mit Brenngasen aus Kohle- und
Schwerölvergasung", VDI
Berichte 1566, VDI Conference Essen, Germany.
[7] Jericha, H., Göttlich,
E., 2002, "Conceptual Design
for an Industrial Prototype Graz Cycle Power Plant", ASME Paper
2002-GT-30118, ASME Turbo Expo 2002,
[8] Jericha, H., Göttlich, E., Sanz, W., Heitmeir, F., 2003, "Design Optimisation of the Graz Cycle Prototype Plant",
ASME Paper 2003-GT-38120, ASME Turbo Expo 2003,
[9] Heitmeir, F., Sanz, W., Göttlich, E., Jericha H., 2003, "The Graz
Cycle – A Zero Emission Power Plant of Highest Efficiency", XXXV
Kraftwerkstechnisches Kolloquium,
[10] Jericha, H., Sanz, W., Pieringer, P., Göttlich E., Erroi, P., 2004, "Konstruktion der ersten Stufe der HTT-Gasturbine für den Graz Cycle
Prototyp“ (in German), VDI Conference Leverkusen, Germany.
[11] Sanz., W., Jericha,
H., Moser, M., Heitmeir, F., 2004, "Thermodynamic
and Economic Investigation of an Improved Graz Cycle Power Plant for CO2
Capture", ASME Paper GT2004-53722, ASME Turbo Expo 2004, Vienna,
Austria. (Conference
presentation)
[12] Moser, M., 2004, "Thermodynamische und wirtschaftliche Optimierung des Graz Cycle", (in German), Master thesis,
Graz University of Technology. (nominated
for best TU-Graz Master thesis award of 2004)
[13] Luckel, F., 2004, "Weiterentwicklung des Graz Cycle
und der Vergleich mit anderen CO2-Rückhaltekonzepten", (in German), Master
thesis, Graz University of Technology.
[14] Erroi, P., 2004, "Strömungssimulation der ersten Stufe der
Hochtemperaturturbine des Graz-Cycles", (in
German), Master thesis, Graz University of
Technology. (nominated
for best TU-Graz Master thesis award of 2004)
[15] Sanz, W., Jericha,
H., Luckel, F., Göttlich,
E., Heitmeir, F., 2005, "A Further
Step Towards a Graz Cycle Power Plant for CO2 Capture", ASME Paper
GT2005-68456, ASME Turbo Expo 2005, Reno-Tahoe, Nevada, USA. (Conference
presentation)
[16] Heitmeir, F., Jericha,
H., 2005, "Turbomachinery design for the Graz cycle: an
optimized power plant concept for CO2 retention", Proceedings
of the Institution of Mechanical Engineers Part A: Journal of Power and Energy,
Volume 219, Number 2, pp. 147-158(12). (DOI)
[17] Jericha, H., Sanz, W., Göttlich, E., 2006,
"Design
Concept for Large Output Graz Cycle Gas Turbines", ASME Paper
GT2006-90032, ASME Turbo Expo 2006,
[18] Jericha, H., Sanz, W., Göttlich E., 2006,
"Gasturbine mit CO2-Rückhaltung
– 490 MW (Oxyfuel-System Graz Cycle)“ (in German), VDI Conference Leverkusen,
Germany (Conference
presentation)
[19] Jericha, H., Sanz, W., Göttlich E., 2007,
"Gas
Turbine with CO2 Retention – 400 MW Oxyfuel-System
Graz Cycle“, Paper No. 168, CIMAC Conference 2007, Vienna, Austria (Conference
presentation)
[20] Sanz, W., Jericha, H., Bauer,
B., Göttlich E., 2007,
"Qualitative
and Quantitative Comparison of Two Promising Oxy-Fuel Power Cycles for CO2
Capture“, ASME Paper GT2007-27375, ASME Turbo Expo 2007, Montreal,
Canada (Conference
presentation). Also published in: Journal of Engineering
for Gas Turbines and Power, Volume 130, Issue 3, May 2008. (DOI)
[21] Jericha, H., Sanz, W., Göttlich E., Neumayer, F., 2008, "Design Details of a 600 MW Graz Cycle
Thermal Power Plant for CO2 Capture“, ASME Paper GT2008-50515, ASME Turbo Expo
2008, Berlin, Germany (Conference
presentation)
[22] Jericha, H., Sanz, W., Göttlich E., Neumayer, F., 2008, "Mit Überschallstufen und ICS-Dampfkühlung zur 600 MW Oxyfuel-Graz-Cycle-Einheit“ (in
German), VDI Conference Leverkusen, Germany (Conference
presentation)
[23] Sanz, W., Mayr M., Jericha, H., 2010, "Thermodynamic and Economic
Evaluation of an IGCC Plant Based on the Graz Cycle for CO2 Capture“, ASME Paper GT2010-22189, ASME Turbo Expo
2010, Glasgow, UK (Conference
presentation)
[24] Sanz, W., Hustad, C.-W., Jericha, H., 2011, "First
Generation Graz Cycle Plant for Near-Term Deployment“, ASME Paper
GT2011-45135, ASME Turbo Expo 2011,
The list
below is by no far an exhaustive list of publications mentioning the
-
Mori, H., Sugishita, H., Uematsu, K., 1998, "A Study of 50MW Hydrogen Combustion
Turbines", XII World Hydrogen Energy Conference. (HTML)
-
Bolland, B., Kvamsdal, H.M., Boden, J.C., 2001,
"A Thermodynamic Comparison of the Oxy-Fule
Power Cycles, Water-cycle, Graz-Cycle and Matiant-Cycle",
International Conference on Power Generation and Sustainable Development,
-
Celano A., 2002,
"Comparison of near Zero CO2 Emission Power Plants on CO2/H2O
Mixture", Doctoral Thesis,
-
Kail, C., Haberberger, G., 2002, "Kohlendioxid-Rückhaltung und Wirkungsgraderhöhung durch
interne Zusatzfeuerung bei Dampfkraftwerken", (in German), VDI Berichte
1714. (PDF)
-
Miller, A.,
Lewandowski, J., Badyda, K., Kiryk,
S., Milewski, J.,
-
Mathieu, P., 2003, "Zero Emission Technologies: An Option
for Climate Change Mitigation", Third Nordic Minisymposium
on Carbon Dioxide Capture and Storage,
-
Gupta, M., Coyle,
-
Ito,
S., Saeki, H., Inomata, A., Ootomo, F., Yamashita,
K., Fukuyama, Y., Koda, E., Takehashi,
T., Sato, M., Koyama, M., Ninomiya, T., 2005, "Conceptual Design and Cooling Blade Development of 1700°C
Class High-Temperature Gas Turbine", Journal of Engineering for Gas
Turbines and Power, Volume 127, Issue 2, pp. 358-368. (DOI)
-
Anheden, M., Yan, J., De Smedt, G., 2005, "Denitrogenation
(or Oxyfuel Concepts)", Oil & Gas Science
and Technology – Rev. IFP, Vol. 60 (2005), No. 3, pp. 485-495. (PDF)
-
Gou,
C., Cai, R., Hong, H., 2006, "An Advanced Oxy-Fuel Power Cycle with High Efficiency",
Proceedings of the Institution of Mechanical Engineers Part A: Journal of Power
and Energy, Volume 220, Number 4, pp. 315-325(11). (DOI)
-
ENCAP, 2006, “Second Newsletter of ENCAP
Project” (PDF)
-
Franco, F., Mina, T., Woolatt, G., Rost, M., Bolland, O., 2006, “Characteristics of
Cycle Components for CO2 Capture”, Proceedings of 8th International Conference
on Greenhouse Gas Control Technologies,
-
Kvamsdal, H.M., Bolland, O., Maurstad, O., Jordal, K., 2006,
"A Qualitative Comparison of Gas Turbine Cycles with CO2 Capture", Proceedings of 8th International Conference on
Greenhouse Gas Control Technologies,
-
Zero Emissions
Platform, 2011, “The
Costs of CO2 Capture – Post-demonstration CCS in EU”, Report by the
European Technology Platform for Zero Emission Fossil Fuel Power Plants (PDF)
-
Zhang, N., Lior, N., 2008,
"Comparative Study of Two Low CO2 Emission Power Generation System Options
With Natural Gas Reforming", Journal of Engineering for Gas Turbines and
Power, Volume 130, Issue 5, September 2008. (DOI)
-
VGB PowerTech Service GmbH, " CO2 Capture and Storage
– VGB Report on the State of the Art", VGB PowerTech
Service GmbH, August 2004. (PDF)
This web page is maintained by
Wolfgang Sanz,
Professor at the Institute for Thermal
Turbomachinery and Machine Dynamics (TTM), Graz University of Technology.
Contact: wolfgang.sanz@TUGraz.at
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