Standard

Heat pipe : A simple one-dimensional model and an experimental study. / Cheverda, V. V.; Vozhakov, I. S.; Ronshin, F. V.

In: Journal of Physics: Conference Series, Vol. 1369, No. 1, 012054, 26.11.2019.

Research output: Contribution to journal › Conference article › peer-review

Harvard

Cheverda, VV, Vozhakov, IS & Ronshin, FV 2019, 'Heat pipe: A simple one-dimensional model and an experimental study', Journal of Physics: Conference Series, vol. 1369, no. 1, 012054. https://doi.org/10.1088/1742-6596/1369/1/012054

APA

Cheverda, V. V., Vozhakov, I. S., & Ronshin, F. V. (2019). Heat pipe: A simple one-dimensional model and an experimental study. Journal of Physics: Conference Series, 1369(1), [012054]. https://doi.org/10.1088/1742-6596/1369/1/012054

Vancouver

Cheverda VV, Vozhakov IS, Ronshin FV. Heat pipe: A simple one-dimensional model and an experimental study. Journal of Physics: Conference Series. 2019 Nov 26;1369(1):012054. doi: 10.1088/1742-6596/1369/1/012054

Author

Cheverda, V. V. ; Vozhakov, I. S. ; Ronshin, F. V. / Heat pipe : A simple one-dimensional model and an experimental study. In: Journal of Physics: Conference Series. 2019 ; Vol. 1369, No. 1.

BibTeX

@article{3e86479ab23b48ea9e99e2ad5db22cd8,
title = "Heat pipe: A simple one-dimensional model and an experimental study",
abstract = "In this work the authors proposed to use 1-D model for heat and masstransfer calculations inside a porous heat pipe. Several limits are taken in to account: Sound, boiling, capillary and dry out of evaporator. To calculate the heat flow, we analyzed processes in four zones: The evaporator, the condenser, the porous body in which fluid flows, and the cavity in which steam flows. We assume that in the evaporator all the incoming liquid evaporates, and in the condenser, all the vapor condenses. The liquid and the vapor are in a state of saturation and, therefore, the pressure in the condenser and the evaporator is equal to the saturation pressure. The good agreement between theoretical and experimental results is observed.",
author = "Cheverda, {V. V.} and Vozhakov, {I. S.} and Ronshin, {F. V.}",
year = "2019",
month = nov,
day = "26",
doi = "10.1088/1742-6596/1369/1/012054",
language = "English",
volume = "1369",
journal = "Journal of Physics: Conference Series",
issn = "1742-6588",
publisher = "IOP Publishing Ltd.",
number = "1",
note = "5th International Workshop on Heat/Mass Transfer Advances for Energy Conservation and Pollution Control, IWHT 2019 ; Conference date: 13-08-2019 Through 16-08-2019",

}

RIS

TY - JOUR

T1 - Heat pipe

T2 - 5th International Workshop on Heat/Mass Transfer Advances for Energy Conservation and Pollution Control, IWHT 2019

AU - Cheverda, V. V.

AU - Vozhakov, I. S.

AU - Ronshin, F. V.

PY - 2019/11/26

Y1 - 2019/11/26

N2 - In this work the authors proposed to use 1-D model for heat and masstransfer calculations inside a porous heat pipe. Several limits are taken in to account: Sound, boiling, capillary and dry out of evaporator. To calculate the heat flow, we analyzed processes in four zones: The evaporator, the condenser, the porous body in which fluid flows, and the cavity in which steam flows. We assume that in the evaporator all the incoming liquid evaporates, and in the condenser, all the vapor condenses. The liquid and the vapor are in a state of saturation and, therefore, the pressure in the condenser and the evaporator is equal to the saturation pressure. The good agreement between theoretical and experimental results is observed.

AB - In this work the authors proposed to use 1-D model for heat and masstransfer calculations inside a porous heat pipe. Several limits are taken in to account: Sound, boiling, capillary and dry out of evaporator. To calculate the heat flow, we analyzed processes in four zones: The evaporator, the condenser, the porous body in which fluid flows, and the cavity in which steam flows. We assume that in the evaporator all the incoming liquid evaporates, and in the condenser, all the vapor condenses. The liquid and the vapor are in a state of saturation and, therefore, the pressure in the condenser and the evaporator is equal to the saturation pressure. The good agreement between theoretical and experimental results is observed.

UR - http://www.scopus.com/inward/record.url?scp=85079355928&partnerID=8YFLogxK

U2 - 10.1088/1742-6596/1369/1/012054

DO - 10.1088/1742-6596/1369/1/012054

M3 - Conference article

AN - SCOPUS:85079355928

VL - 1369

JO - Journal of Physics: Conference Series

JF - Journal of Physics: Conference Series

SN - 1742-6588

IS - 1

M1 - 012054

Y2 - 13 August 2019 through 16 August 2019

ER -

ID: 23523691