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    Impact of HSPBT blade angle on gas phase hydrodynamics in a gas–liquid stirred tank

    Access Status
    Fulltext not available
    Authors
    Prakash, B.
    Shah, Milin
    Pareek, Vishnu
    Utikar, Ranjeet
    Date
    2018
    Type
    Journal Article
    
    Metadata
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    Citation
    Prakash, B. and Shah, M. and Pareek, V. and Utikar, R. 2018. Impact of HSPBT blade angle on gas phase hydrodynamics in a gas–liquid stirred tank. Chemical Engineering Research and Design. 130: pp. 219-229.
    Source Title
    Chemical Engineering Research and Design
    DOI
    10.1016/j.cherd.2017.12.028
    ISSN
    0263-8762
    School
    WASM: Minerals, Energy and Chemical Engineering (WASM-MECE)
    URI
    http://hdl.handle.net/20.500.11937/66886
    Collection
    • Curtin Research Publications
    Abstract

    For gas dispersion applications in stirred tanks, standard pitched blade turbine (PBT) with 45° blade angle is widely used. However, the standard PBT suffers from low pumping efficiency as well as high torque instability when a large volume of gas is to be dispersed. Thus, high solidity pitched blade turbine (HSPBT), which has a higher blade to impeller area has been developed. The performance of HSPBT relies on the impeller blade angle that governs impeller shear, break up of bubbles, and pumping efficiency. For HSPBT, detailed experimental data is not available, which hinders its design optimization. This study investigates the effect of blade angle (30°, 45°, and 60°) on gas holdup, power consumption, and bubble properties (size, frequency, and velocity) in a pilot-scale stirred tank using optical probe measurements. Increasing the blade angle from 30° to 60° resulted in increase in overall gas holdup and power consumption. For 30° blade angle, the bubble frequency was approximately three times higher at impeller trailing edge compared to the tank center and wall; whereas average bubble velocity was 15–20% lower at the trailing edge. Increasing the blade angle to 60° resulted in further increase in bubble frequency and drop in bubble velocity at the trailing edge. Wide chord length distribution (1–5 cm) was observed at the tank center; whereas narrower distribution in chord length (0–1 cm) was observed at the impeller trailing edge. Further analysis of bubble population shown that the contribution of small bubbles to overall gas holdup was highest using HSPBT45°. Higher gas holdup and finer bubbles were observed for HSPBT45° compared to HSPBT60° at reasonably lower power input.

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