| dc.creator |
ÇALIŞKAN, HAKAN |
|
| dc.creator |
ŞÖHRET, Yasin |
|
| dc.creator |
Ekici, Selcuk |
|
| dc.date |
2022-09-01T00:00:00Z |
|
| dc.date.accessioned |
2023-01-09T12:04:30Z |
|
| dc.date.available |
2023-01-09T12:04:30Z |
|
| dc.identifier |
7b8ff0d7-1633-4b82-acf8-5d2135b30b09 |
|
| dc.identifier |
10.1016/j.jppr.2022.07.002 |
|
| dc.identifier |
https://avesis.sdu.edu.tr/publication/details/7b8ff0d7-1633-4b82-acf8-5d2135b30b09/oai |
|
| dc.identifier.uri |
http://acikerisim.sdu.edu.tr/xmlui/handle/123456789/98033 |
|
| dc.description |
In this study, exergy dynamic and advanced exergy analyses are applied to the turbojet engine to assess its mexogenous, endogenous, exogenous, avoidable and unavoidable exergies under the environment conditions of 15 degrees C temperature and 1 bar pressure. The maximum exergy point in the turbojet engine is found for the combustor in which C11H23 (Jet-A1) fuel is combusted with air, while the minimum one is determined for the air compressor head where the free air enters. The combustion chamber has the maximum fuel, product and irreversibility rates and the air compressor has the minimum fuel and product ex-ergy values, while the minimum irreversibility is found for the turbine. Maximum improvement potential rate is found for the combustion chamber (5141.27 kW), while minimum rate is deter-mined for the turbine of system (6.95 kW). Also, the turbine component has the highest exergy efficiency (97.20%) due to its expansion process, while combustion chamber component has the lowest exergy efficiency (55.39%) due to low efficient combustion process of the fuel. Furthermore, the mexogenous exergy destructions from maximum to minimum are found for |
|
| dc.language |
eng |
|
| dc.rights |
info:eu-repo/semantics/closedAccess |
|
| dc.title |
Advanced exergy analysis of the turbojet engine main components considering mexogenous, endogenous, exegenous, avoidable and unavoidable exergy destructions |
|
| dc.type |
info:eu-repo/semantics/article |
|