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Laser Doppler Anemometry of Cavitating Hydrofoil in a Slit. / Kravtsova, A. Yu; Kulikov, D. V.; Lanshakov, D. A. et al.

In: Journal of Engineering Thermophysics, Vol. 33, No. 3, 18.09.2024, p. 646-651.

Research output: Contribution to journal › Article › peer-review

Harvard

Kravtsova, AY, Kulikov, DV, Lanshakov, DA, Kashkarova, MV & Dvoinishnikov, SV 2024, 'Laser Doppler Anemometry of Cavitating Hydrofoil in a Slit', Journal of Engineering Thermophysics, vol. 33, no. 3, pp. 646-651. https://doi.org/10.1134/S1810232824030160

APA

Kravtsova, A. Y., Kulikov, D. V., Lanshakov, D. A., Kashkarova, M. V., & Dvoinishnikov, S. V. (2024). Laser Doppler Anemometry of Cavitating Hydrofoil in a Slit. Journal of Engineering Thermophysics, 33(3), 646-651. https://doi.org/10.1134/S1810232824030160

Vancouver

Kravtsova AY, Kulikov DV, Lanshakov DA, Kashkarova MV, Dvoinishnikov SV. Laser Doppler Anemometry of Cavitating Hydrofoil in a Slit. Journal of Engineering Thermophysics. 2024 Sept 18;33(3):646-651. doi: 10.1134/S1810232824030160

Author

Kravtsova, A. Yu ; Kulikov, D. V. ; Lanshakov, D. A. et al. / Laser Doppler Anemometry of Cavitating Hydrofoil in a Slit. In: Journal of Engineering Thermophysics. 2024 ; Vol. 33, No. 3. pp. 646-651.

BibTeX

@article{a5d94dd340b84c3abb9d70c36101f555,
title = "Laser Doppler Anemometry of Cavitating Hydrofoil in a Slit",
abstract = "Laser Doppler anemometry (LDA) is one of the main non-contact methods for measuring the velocity characteristics of flows and pressure pulsations. Determining the quantitative patterns of the flow of multiphase liquids in small-sized channels is known to be a difficult task. The authors demonstrate the eventual use of LDA to study cavitation flows in slits with a height of 1.2 mm. The cavitation flow is created by means of the NACA0012 hydrofoil. The experimental equipment is positioned using a micro-displacement device. The distortion of the luminous flux through the channel walls is taken into account. This paper presents an algorithm for searching the central region of the slit. A method for filtering noise effects is described. The results of measuring the average flow velocity near the cavitating hydrofoil in the slit are provided in the article.",
author = "Kravtsova, {A. Yu} and Kulikov, {D. V.} and Lanshakov, {D. A.} and Kashkarova, {M. V.} and Dvoinishnikov, {S. V.}",
year = "2024",
month = sep,
day = "18",
doi = "10.1134/S1810232824030160",
language = "English",
volume = "33",
pages = "646--651",
journal = "Journal of Engineering Thermophysics",
issn = "1810-2328",
publisher = "Maik Nauka-Interperiodica Publishing",
number = "3",

}

RIS

TY - JOUR

T1 - Laser Doppler Anemometry of Cavitating Hydrofoil in a Slit

AU - Kravtsova, A. Yu

AU - Kulikov, D. V.

AU - Lanshakov, D. A.

AU - Kashkarova, M. V.

AU - Dvoinishnikov, S. V.

PY - 2024/9/18

Y1 - 2024/9/18

N2 - Laser Doppler anemometry (LDA) is one of the main non-contact methods for measuring the velocity characteristics of flows and pressure pulsations. Determining the quantitative patterns of the flow of multiphase liquids in small-sized channels is known to be a difficult task. The authors demonstrate the eventual use of LDA to study cavitation flows in slits with a height of 1.2 mm. The cavitation flow is created by means of the NACA0012 hydrofoil. The experimental equipment is positioned using a micro-displacement device. The distortion of the luminous flux through the channel walls is taken into account. This paper presents an algorithm for searching the central region of the slit. A method for filtering noise effects is described. The results of measuring the average flow velocity near the cavitating hydrofoil in the slit are provided in the article.

AB - Laser Doppler anemometry (LDA) is one of the main non-contact methods for measuring the velocity characteristics of flows and pressure pulsations. Determining the quantitative patterns of the flow of multiphase liquids in small-sized channels is known to be a difficult task. The authors demonstrate the eventual use of LDA to study cavitation flows in slits with a height of 1.2 mm. The cavitation flow is created by means of the NACA0012 hydrofoil. The experimental equipment is positioned using a micro-displacement device. The distortion of the luminous flux through the channel walls is taken into account. This paper presents an algorithm for searching the central region of the slit. A method for filtering noise effects is described. The results of measuring the average flow velocity near the cavitating hydrofoil in the slit are provided in the article.

UR - https://www.mendeley.com/catalogue/0afb66cb-ccb1-3734-b9ae-5f44cfb90015/

U2 - 10.1134/S1810232824030160

DO - 10.1134/S1810232824030160

M3 - Article

VL - 33

SP - 646

EP - 651

JO - Journal of Engineering Thermophysics

JF - Journal of Engineering Thermophysics

SN - 1810-2328

IS - 3

ER -

ID: 60813952