Multi-Control-Volume Analysis of the Compression Process in a High-Temperature Root's Type Compressor
In this study we have modeled a high-temperature Root's type compressor and compared predicted results with measurements. Compression process is modeled using multiple control volumes. Initially, there are two control volumes connected by an “expansion nozzle” naturally formed by the rotor tip...
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2004-01-01
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Series: | International Journal of Rotating Machinery |
Online Access: | http://dx.doi.org/10.1155/S1023621X04000053 |
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doaj-a944b9ca29484277b81f7e9f37975a742020-11-24T23:13:53ZengHindawi LimitedInternational Journal of Rotating Machinery1023-621X2004-01-01101455310.1155/S1023621X04000053Multi-Control-Volume Analysis of the Compression Process in a High-Temperature Root's Type CompressorDavid I. Blekhman0Joseph C. Mollendorf1James D. Felske2John A. Lordi3Padnos School of Engineering, Grand Valley State University, 301 W. Fulton St., Grand Rapids 49504-6431, MI, USAMechanical and Aerospace Engineering Department, State University of New York at Buffalo, Buffalo, New York, USAMechanical and Aerospace Engineering Department, State University of New York at Buffalo, Buffalo, New York, USAMechanical and Aerospace Engineering Department, State University of New York at Buffalo, Buffalo, New York, USAIn this study we have modeled a high-temperature Root's type compressor and compared predicted results with measurements. Compression process is modeled using multiple control volumes. Initially, there are two control volumes connected by an “expansion nozzle” naturally formed by the rotor tip and the blower casing. The “nozzle” has time-varying geometry and is modeled to allow transition from choked to non-choked flow. The well-filling process is modeled via expansion of the compressed gas from the high-pressure reservoir into the well through this “nozzle.” When the pressures in the well and reservoir equalize, the “passive” part of the compression process is taken to be complete. At this point, the gas in the well is assumed to be fully-mixed and the two control volumes are subsequently considered as one. Then the “active” part of compression takes place. Numerical computations are shown to agree well with the experimental data.http://dx.doi.org/10.1155/S1023621X04000053 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
David I. Blekhman Joseph C. Mollendorf James D. Felske John A. Lordi |
spellingShingle |
David I. Blekhman Joseph C. Mollendorf James D. Felske John A. Lordi Multi-Control-Volume Analysis of the Compression Process in a High-Temperature Root's Type Compressor International Journal of Rotating Machinery |
author_facet |
David I. Blekhman Joseph C. Mollendorf James D. Felske John A. Lordi |
author_sort |
David I. Blekhman |
title |
Multi-Control-Volume Analysis of the Compression Process in a High-Temperature Root's Type Compressor |
title_short |
Multi-Control-Volume Analysis of the Compression Process in a High-Temperature Root's Type Compressor |
title_full |
Multi-Control-Volume Analysis of the Compression Process in a High-Temperature Root's Type Compressor |
title_fullStr |
Multi-Control-Volume Analysis of the Compression Process in a High-Temperature Root's Type Compressor |
title_full_unstemmed |
Multi-Control-Volume Analysis of the Compression Process in a High-Temperature Root's Type Compressor |
title_sort |
multi-control-volume analysis of the compression process in a high-temperature root's type compressor |
publisher |
Hindawi Limited |
series |
International Journal of Rotating Machinery |
issn |
1023-621X |
publishDate |
2004-01-01 |
description |
In this study we have modeled a high-temperature Root's type compressor and compared predicted results with measurements. Compression process is modeled using multiple control volumes. Initially, there are two control volumes connected
by an “expansion nozzle” naturally formed by the rotor tip and the blower casing. The “nozzle” has time-varying geometry and is modeled to allow transition from choked to non-choked flow. The well-filling process is modeled via expansion
of the compressed gas from the high-pressure reservoir into the well through this “nozzle.” When the pressures in the well and reservoir equalize, the “passive” part of the compression process is taken to be complete. At this point, the gas in the well is assumed to be fully-mixed and the two control volumes are subsequently considered as one. Then the “active” part of compression takes place. Numerical computations are shown to agree well with the experimental data. |
url |
http://dx.doi.org/10.1155/S1023621X04000053 |
work_keys_str_mv |
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1725596400384737280 |