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Vortex-meter design: The influence of shedding-body geometry on shedding characteristics
KTH, Skolan för teknikvetenskap (SCI), Mekanik.
KTH, Skolan för teknikvetenskap (SCI), Mekanik, Strömningsfysik.
KTH, Skolan för teknikvetenskap (SCI), Mekanik, Strömningsfysik.ORCID-id: 0000-0002-1146-3241
2018 (Engelska)Ingår i: Flow Measurement and Instrumentation, ISSN 0955-5986, E-ISSN 1873-6998, Vol. 59, s. 88-102Artikel i tidskrift (Refereegranskat) Published
Abstract [en]

The periodic vortex shedding from bluff bodies may be used in flow metering applications. However, because the bluff-body is highly confined (typically in a pipe) the shed vortices may interact with the pipe wall; causing an undesirable non-linear behaviour. An experimental investigation has been conducted; examining the vortex-shedding characteristics of highly confined bluff-bodies in pipe flow, at high Reynolds number (ReD=4.4×104 to 4.4×105). The bluff-bodies were comprised of a forebody and tail; both of which affected the primary-shedding characteristics. The shedders typically produced two unsteady modes: Mode-I was associated with the vortex shedding and mode-II resulted from a separation of the pipe-wall boundary layer. The mode-I behaviour allowed two classes of shedder to be defined: long-tails and short-tails. Modes I and II interacted, particularly for long-tailed geometries. When the length-scale of mode-II exceeded 0.8κ (where κ is the physical scale of the primary shedding vortex), mode-II disrupted mode-I, as the mode-frequency ratio (fII/fI) approached an integer value. The coupling of modes I and II caused mode-I to deviate from its preferred Strouhal number. When the deviation exceeded 25–30%, mode-I locked on to the mode-II frequency. This did not happen for short-tailed geometries, as the length-scale of mode-I was always dominant. Mode-coupling for short-tails occurred only when the mode frequencies were equal. 

Ort, förlag, år, upplaga, sidor
Elsevier Ltd , 2018. Vol. 59, s. 88-102
Nyckelord [en]
Bluff-body, Compressible, Frequency-characteristic, Splitter-plate, Vortex-meter, Vortex-shedding, Boundary layer flow, Boundary layers, Geometry, Reynolds number, Vortex shedding, Bluff body, Coupling of modes, Experimental investigations, Frequency characteristic, High Reynolds number, Nonlinear behaviours, Splitter plates, Vortex flow
Nationell ämneskategori
Maskinteknik
Identifikatorer
URN: urn:nbn:se:kth:diva-223133DOI: 10.1016/j.flowmeasinst.2017.12.004ISI: 000428102800012Scopus ID: 2-s2.0-85039164249OAI: oai:DiVA.org:kth-223133DiVA, id: diva2:1193465
Anmärkning

QC 20190423

Tillgänglig från: 2018-03-27 Skapad: 2018-03-27 Senast uppdaterad: 2024-03-18Bibliografiskt granskad
Ingår i avhandling
1. Dynamics of Exhaust Valve Flows and Confined Bluff Body Vortex Shedding
Öppna denna publikation i ny flik eller fönster >>Dynamics of Exhaust Valve Flows and Confined Bluff Body Vortex Shedding
2019 (Engelska)Doktorsavhandling, sammanläggning (Övrigt vetenskapligt)
Alternativ titel[sv]
Dynamik för avgasventilflöden och virvelavlösning från trubbiga kroppar
Abstract [en]

This thesis can be divided into two interconnected topics; engine exhaust-valve flows and confined bluff-body vortex shedding. When optimising engine flow systems it is common to use low order simulation tools that require empirical inputs, for instance with respect to flow losses across the exhaust valves. These are typically obtained from experiments at low pressure ratios and for steady flow, assuming the flow to be insensitive to the pressure ratio and that it can be considered as quasi-steady. Here these two assumptions are challenged by comparing measurements of mass-flow rates under steady and dynamic conditions at realistic pressure ratios. The experiments with a static valve were carried out using a high-pressure flow bench at cylinder pressures up to 500 kPa. For the dynamic-valve experiments the transient flow rate during the blowdown phase of an initially pressurised cylinder was determined. Here a linear motor actuated the valve to obtain equivalent engine speeds in the range 800–1350 rpm. It was shown that neither of the above mentioned assumptions are valid and a new non-dimensional quantification of the steadiness of the process was formulated. Furthermore it was shown through Schlieren visualisation that the shock structures in the exhaust port differ depending on if the system dynamics are included or not. The study shows that reliable results of flow losses past exhaust valves can only be obtained in dynamic experiments at representative pressure ratios. The second topic arose from the need to monitor time-resolved mass-flow rates in conduits. A mass-flow meter based on vortex shedding from bluff bodies was designed where microphones are used to detect the shedding frequency. It consists of a forebody and a downstream mounted tail and the system was shown to be capable of measuring pulsating flow rates. Furthermore, the flow topology associated with different forebody and splitter plates has been characterised, through visualisation of the flow behind the shedder and on the splitter plate. It has been shown that for long splitter plates a “horse shoe” like vortex, which attaches to the tail, is formed. It has also been shown that another energetic mode (denoted mode-II) can interact with and disrupt the primary vortex formation. A hypothesis for the appearance of mode-II has been formulated, linking it to the periodic separation of the boundary layer at the conduit wall.

Ort, förlag, år, upplaga, sidor
KTH Royal Institute of Technology, 2019. s. 77
Serie
TRITA-MEK, ISSN 0348-467X ; 2019:16
Nationell ämneskategori
Strömningsmekanik
Forskningsämne
Teknisk mekanik
Identifikatorer
urn:nbn:se:kth:diva-249702 (URN)978-91-7873-159-6 (ISBN)
Disputation
2019-05-24, F3, Stockholm, 10:15 (Engelska)
Opponent
Handledare
Anmärkning

QC 20190423

Tillgänglig från: 2019-04-23 Skapad: 2019-04-17 Senast uppdaterad: 2025-02-09Bibliografiskt granskad

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Ford, C. L.Winroth, P. MarcusAlfredsson, P. Henrik
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