| 000 | 03967nlm1a2200445 4500 | ||
|---|---|---|---|
| 001 | 664707 | ||
| 005 | 20231030041939.0 | ||
| 035 | _a(RuTPU)RU\TPU\network\35891 | ||
| 035 | _aRU\TPU\network\34676 | ||
| 090 | _a664707 | ||
| 100 | _a20210514a2021 k y0engy50 ba | ||
| 101 | 0 | _aeng | |
| 102 | _aNL | ||
| 135 | _adrcn ---uucaa | ||
| 181 | 0 | _ai | |
| 182 | 0 | _ab | |
| 200 | 1 |
_aCollisions of water droplets in the high-temperature air _fP. Tkachenko, N. E. Shlegel, P. A. Strizhak |
|
| 203 |
_aText _celectronic |
||
| 300 | _aTitle screen | ||
| 320 | _a[References: 38 tit.] | ||
| 330 | _aThe paper presents experimental research findings on the integral characteristics of the interaction of water droplets in a gas heated to high temperatures. An induction heater with an internal volume of about 0.13 m3 was used. It was fitted with quartz glass observation windows to record the characteristics of droplet motion before and after collisions. Air was used as a gas medium in the inductor. The parameters were varied in the following ranges: the air medium temperature 20–700 °?, the initial radius of droplets 0.3–0.9 mm, their velocity 0.1–7 m/s and impact angle 0–90°. At high gas temperatures, droplets were two-phase objects, because vapor bubbles formed in their near-surface layer. Frames with four collision regimes (coalescence, separation, disruption and bounce) were recorded. There were significant differences in the transformation of the water droplet surface and in the interaction of droplets with each other at various gas temperatures in the heating chamber. It has been shown that the growth of the air temperature increases the droplet lifetime and causes them to deviate from the spherical shape. The effect of the gas temperature on the position of droplet collision boundaries was determined with due consideration of the relative linear interaction parameter and the Weber number. When the gas temperature increases, two areas may form, corresponding to the bounce of droplets on the collision regime map. Differences were established in the number and dimensions of secondary water droplets formed from the collision of two initial ones. The total surface areas of liquid before and after droplet collisions were calculated. | ||
| 333 | _aРежим доступа: по договору с организацией-держателем ресурса | ||
| 461 | _tInternational Journal of Heat and Mass Transfer | ||
| 463 |
_tVol. 170 _v[121011, 13 p.] _d2021 |
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| 610 | 1 | _aэлектронный ресурс | |
| 610 | 1 | _aтруды учёных ТПУ | |
| 610 | 1 | _awater droplets | |
| 610 | 1 | _ainteraction regimes | |
| 610 | 1 | _aregime map | |
| 610 | 1 | _ahigh-temperature gas medium | |
| 610 | 1 | _achild droplets | |
| 610 | 1 | _aкапли воды | |
| 610 | 1 | _aрежимы взаимодействия | |
| 700 | 1 |
_aTkachenko _bP. _cspecialist in the field of heat and power engineering _cResearch Engineer of Tomsk Polytechnic University _f1996- _gPavel _2stltpush _3(RuTPU)RU\TPU\pers\46849 |
|
| 701 | 1 |
_aShlegel _bN. E. _cspecialist in the field of heat and power engineering _cResearch Engineer of Tomsk Polytechnic University _f1995- _gNikita Evgenjevich _2stltpush _3(RuTPU)RU\TPU\pers\46675 |
|
| 701 | 1 |
_aStrizhak _bP. A. _cSpecialist in the field of heat power energy _cDoctor of Physical and Mathematical Sciences (DSc), Professor of Tomsk Polytechnic University (TPU) _f1985- _gPavel Alexandrovich _2stltpush _3(RuTPU)RU\TPU\pers\30871 |
|
| 712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет _bИнженерная школа энергетики _bНаучно-образовательный центр И. Н. Бутакова (НОЦ И. Н. Бутакова) _h8025 _2stltpush _3(RuTPU)RU\TPU\col\23504 |
| 801 | 2 |
_aRU _b63413507 _c20210514 _gRCR |
|
| 856 | 4 | _uhttps://doi.org/10.1016/j.ijheatmasstransfer.2021.121011 | |
| 942 | _cCF | ||