THERMODYNAMIC CYCLE OF REGASIFICATION OF LIQUEFIED GASES WITH PRODUCTION OF MECHANICAL ENERGY
DOI:
https://doi.org/10.15421/jchemtech.v31i4.294929Keywords:
liquefied gases, regasification terminals, regasification process, improvement of the process of regasificationAbstract
Transportation, storage and use of liquefied gases occupy a significant part in the world gas industry and maintain a tendency to increase. For economically justified maritime refrigerator transportation, the gases in the terminals of shipment are liquefied. Being delivered to the place of consumption for further use, they are converted into conventional low-pressure gas – regasified. Now this process is carried out in conventional heat exchangers, which are heated by natural sources of heat or specially preheated coolants. Liquefied gases similarly to the compressed mechanical spring contain a large amount of potential energy accumulated during liquefaction. This energy is not used in the current technological regasification process. The work offers the thermodynamic cycle of liquefied gases in which mechanical energy is obtained. Using the hydrodynamic method of transforming the liquid into a saturated steam and the isochoric process of its overheating in the proposed thermodynamic regasification cycle, the steam is repeatedly overheated and isoentropically expanding in the turbine. Combined, this allows for a lot of mechanical work to be done. Given the low temperature of the refrigeration transport of liquefied gases, the work considers the use of a combined hot heat source: the vapor is heated by the heat of the environment and then overheated to a higher temperature by specially heated water. The thermal calculations of the proposing the thermodynamic cycle of LNG (methane), which is transported at a temperature of minus 161.28 °C, and ethylene at minus 101.77 °C. The calculations performed for methane showed that the use of the method in its regasification at one of the largest regasification terminals in Europe, Barcelona, the capacity of which is 17.1 billion nm3/year, will allow obtaining a hypothetical steam turbine plant capacity of 262 737.90 kW. Therefore, the annual energy production will be 2 295 278 302 kW. This amount of electricity requires 573 820 tons of fuel, provided that the specific fuel consumption of the diesel generator is 0.25 kg/(kW∙h).
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