Nucleation and bubble growth during puffing and micro-explosions incomposite droplets; Fuel; Vol. 340
| Parent link: | Fuel Vol. 340.— 2023.— [126991, 14 p.] |
|---|---|
| Corporate Author: | |
| Other Authors: | , , , |
| Summary: | Title screen Heating of droplets composed of water and fuel is known to lead to internal nucleation and bubble growth that can eventually lead to their puffing and to micro-explosions. In the present paper, we examine the effect of different aspects of bubble growth on the puffing and micro-explosions. Specifically, we address the effects of nucleation temperature and the relative positions of the inner water sub-droplet and the bubble within it. The nucleation temperature of the water sub-droplet is higher than its normal boiling temperature yet lower than its spinodal temperature in most realistic cases. The degree of superheating and the nucleation time depend on the heating rate and the nucleation site density. Higher nucleation temperatures imply larger driving force for the bubble growth. Bubble growth rate is dominated by the degree of superheating, while growth time is dominated by both the degree of superheating and the location of the bubble with respect to the inner and outer interfaces of the composite droplet. It is found that the inertial bubble growth regime is dominant for micron-sized droplets, and thus sensitivity to the modelling of the inertial regime can be of crucial importance to the evaluation of the breakup time for the droplets. The model for puffing and micro-explosion presented in the paper considers an isolated bubble growing at the water/fuel interface at various degrees of superheating, and for a wide range of Jakob numbers. This analysis allows us to assess the sensitivity of bubble growth time to the initial bubble location, and to generalise the previously developed model of the phenomenon taking into account the effect of finite time of bubble growth during the development of puffing/micro-explosion. Режим доступа: по договору с организацией-держателем ресурса |
| Language: | English |
| Published: |
2023
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| Subjects: | |
| Online Access: | https://doi.org/10.1016/j.fuel.2022.126991 |
| Format: | Electronic Book Chapter |
| KOHA link: | https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=669378 |
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| 200 | 1 | |a Nucleation and bubble growth during puffing and micro-explosions incomposite droplets |f Bar-Kohany Tali, D. V. Antonov, P. A. Strizhak, S. S. Sazhin | |
| 203 | |a Text |c electronic | ||
| 300 | |a Title screen | ||
| 320 | |a [References: 52 tit.] | ||
| 330 | |a Heating of droplets composed of water and fuel is known to lead to internal nucleation and bubble growth that can eventually lead to their puffing and to micro-explosions. In the present paper, we examine the effect of different aspects of bubble growth on the puffing and micro-explosions. Specifically, we address the effects of nucleation temperature and the relative positions of the inner water sub-droplet and the bubble within it. The nucleation temperature of the water sub-droplet is higher than its normal boiling temperature yet lower than its spinodal temperature in most realistic cases. The degree of superheating and the nucleation time depend on the heating rate and the nucleation site density. Higher nucleation temperatures imply larger driving force for the bubble growth. Bubble growth rate is dominated by the degree of superheating, while growth time is dominated by both the degree of superheating and the location of the bubble with respect to the inner and outer interfaces of the composite droplet. It is found that the inertial bubble growth regime is dominant for micron-sized droplets, and thus sensitivity to the modelling of the inertial regime can be of crucial importance to the evaluation of the breakup time for the droplets. The model for puffing and micro-explosion presented in the paper considers an isolated bubble growing at the water/fuel interface at various degrees of superheating, and for a wide range of Jakob numbers. This analysis allows us to assess the sensitivity of bubble growth time to the initial bubble location, and to generalise the previously developed model of the phenomenon taking into account the effect of finite time of bubble growth during the development of puffing/micro-explosion. | ||
| 333 | |a Режим доступа: по договору с организацией-держателем ресурса | ||
| 461 | |t Fuel | ||
| 463 | |t Vol. 340 |v [126991, 14 p.] |d 2023 | ||
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| 701 | 0 | |a Bar-Kohany Tali | |
| 701 | 1 | |a Antonov |b D. V. |c specialist in the field of heat and power engineering |c Research Engineer of Tomsk Polytechnic University |f 1996- |g Dmitry Vladimirovich |3 (RuTPU)RU\TPU\pers\46666 | |
| 701 | 1 | |a Strizhak |b P. A. |c Specialist in the field of heat power energy |c Doctor of Physical and Mathematical Sciences (DSc), Professor of Tomsk Polytechnic University (TPU) |f 1985- |g Pavel Alexandrovich |3 (RuTPU)RU\TPU\pers\30871 |9 15117 | |
| 701 | 1 | |a Sazhin |b S. S. |c geophysicist |c Leading researcher at Tomsk Polytechnic University, PhD in Physics and Mathematics |f 1949- |g Sergey Stepanovich |9 88718 | |
| 712 | 0 | 2 | |a Национальный исследовательский Томский политехнический университет |b Инженерная школа энергетики |b Научно-образовательный центр И. Н. Бутакова (НОЦ И. Н. Бутакова) |3 (RuTPU)RU\TPU\col\23504 |
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