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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Main Authors: David I. Blekhman, Joseph C. Mollendorf, James D. Felske, John A. Lordi
Format: Article
Language:English
Published: Hindawi Limited 2004-01-01
Series:International Journal of Rotating Machinery
Online Access:http://dx.doi.org/10.1155/S1023621X04000053
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spelling 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
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