Jan Hrdlička

Dr. Jan Hrdlička

Department of Energy Engineering, Czech Technical University in Prague, 166 07 Prague, Czech Republic
orcid

Research Focus & Metrics

Academic Career Length

18Years (2009-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 February 2016 in Fuel
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Journal Article
Closed access
Jan HrdličkaJan Hrdlička
Jan Hrdlička
PSPavel Skopec
Pavel Skopec
TDTomáš Dlouhý
Tomáš Dlouhý
FHFrantišek Hrdlička
František Hrdlička

1 October 2019 in Journal of the Energy Institute
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Journal Article
Closed access
Jan HrdličkaJan Hrdlička
Jan Hrdlička
TDTomáš Dlouhý
Tomáš Dlouhý

30 July 2021 in Energies
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Journal Article
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SPSimon Pratschner
Simon Pratschner
PSPavel Skopec
Pavel Skopec
Jan HrdličkaJan Hrdlička
Jan Hrdlička
Franz WinterFranz Winter
Franz Winter
A revolution of the global energy industry is without an alternative to solving the climate crisis. However, renewable energy sources typically show significant seasonal and daily fluctuations. This paper provides a system concept model of a decentralized power-to-green methanol plant consisting of a biomass heating plant with a thermal input of 20 MWth. (oxyfuel or air mode), a CO2 processing unit (DeOxo reactor or MEA absorption), an alkaline electrolyzer, a methanol synthesis unit, an air separation unit and a wind park. Applying oxyfuel combustion has the potential to directly utilize O2 generated by the electrolyzer, which was analyzed by varying critical model parameters. A major objective was to determine whether applying oxyfuel combustion has a positive impact on the plant’s power-to-liquid (PtL) efficiency rate. For cases utilizing more than 70% of CO2 generated by the combustion, the oxyfuel’s O2 demand is fully covered by the electrolyzer, making oxyfuel a viable option for large scale applications. Conventional air combustion is recommended for small wind parks and scenarios using surplus electricity. Maximum PtL efficiencies of ηPtL,Oxy = 51.91% and ηPtL,Air = 54.21% can be realized. Additionally, a case study for one year of operation has been conducted yielding an annual output of about 17,000 t/a methanol and 100 GWhth./a thermal energy for an input of 50,500 t/a woodchips and a wind park size of 36 MWp.

1 September 2018 in International Journal of Greenhouse Gas Control
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Journal Article
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MVMatěj Vodička
Matěj Vodička
NHNils Erland L. Haugen
Nils Erland L. Haugen
AGAndrea Gruber
Andrea Gruber
Jan HrdličkaJan Hrdlička
Jan Hrdlička

1 May 2011
Verified
Conference Paper
Closed access
VPViktor Placek
Viktor Placek
BSBohumil Sulc
Bohumil Sulc
SVStanislav Vrana
Stanislav Vrana
Jan HrdličkaJan Hrdlička
Jan Hrdlička
Ján PiteľJán Piteľ
Ján Piteľ
This paper discusses certain specific problems of small-scale biomass combustion control and their investigation. It describes development of an experimental stand based on market available boiler for wooden pellets that has been equipped with special control unit based on a PAC. In the paper is shown elimination of CO peaks appearing after periodical grate sweeping and main effort is focused on replacement of mostly used on/off heat output control by a PI controller. Application of the PI controller has lowered CO emissions during transition states and improved stability of the combustion process.

1 January 2016 in Energy Procedia
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Journal Article
Open access
Jan HrdličkaJan Hrdlička
Jan Hrdlička
PSPavel Skopec
Pavel Skopec
JOJan Opatril
Jan Opatril
TDTomas Dlouhy
Tomas Dlouhy
This paper deals with characterization of the oxyfuel combustion in a bubbling fluidized bed. The paper proposes a calculation procedure to evaluate gas flow streams, adiabatic flame temperature and concentrations of species in the flue gas. The second part describes a laboratory scale 30kW oxyfuel BFB and presents results of experiments with various semi-oxyfuel and full oxyfuel modes. The results are compared with experimental results, the agreement is satisfactory with less than 10% relative difference. Sustaining of similar fluidization regime along all different cases resulted in decrease of the adiabatic flame temperature that had to be compensated by thermal volumetric load increase from 3.3 to 4.1 MW/m3