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首页> 外文期刊>Multiphase science and technology >SATURATION BOILING ON MPC: EFFECTS OF THICKNESS, INCLINATION ANGLE, TRANSIENT BUBBLE GROWTH, AND NUCLEATION SITE DENSITY
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SATURATION BOILING ON MPC: EFFECTS OF THICKNESS, INCLINATION ANGLE, TRANSIENT BUBBLE GROWTH, AND NUCLEATION SITE DENSITY

机译:MPC上的饱和沸腾:厚度,倾角,瞬态气泡生长和晶核密度的影响

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摘要

Saturation pool boiling experiments of PF-5060 dielectric on micro-porous copper (MPC) near atmospheric pressure (~0.085 MPa) have investigated the effects of the inclination angle (θ) and thickness (δ_(MPC)) on the nucleate boiling (NB) heat transfer coefficient (h_(NB)) and critical heat flux (CHF). In the experiments, δ_(MPC) varied from 80 to 230 μm and θ varied from 0° (upward facing) to 180° (downward facing). In addition to enhancing h_(NB), there was no (or a slight) excursion in the surface temperature (<5 K) prior to boiling incipience. Increasing δ_(MPC) from 95 to 230 μm increased the CHF from 22 to 26 W/cm~2. The highest [maximum nucleate boiling (MNB)] heat transfer coefficient (h_(MNB)) near the end of fully developed NB region occurred at lower superheat than at the CHF. Both h_(NB) and h_(MNB) increased with increasing δ_(MPC), peaking at ~171 μm, and then decreased with a further increase in δ_(MPC). They were highest in the upward-facing orientation. The h_(MNB) value (up to ~7.8 W/cm~2•K) decreased slowly with increasing θ to 90°, and then decreased faster to the lowest value at 180°. In the upward-facing orientation h_(NB) was correlated in terms of the applied heat flux (h_(NB) = Aq~B); coefficient A increased linearly from 0.427 to 1.143 as δ_(MPC) increased from 80 to 230 μm, while B increased from 0.522 to a peak of 0.686 at δ_(MPC) ~ 162 μm, and then decreased to 0.573 at δ_(MPC) = 230 μm. The h_(NB) correlation agreed with the data to within ±12%. Also developed was a correlation for the transient bubble growth on MPC at low heat flux (<0.48 W/cm~2). This correlation agreed to within ±5% with measurements from footings recorded using a video camera at 210 frames per second. The bubble's departure diameter (D_d = 431 ± 7 μm) and detachment frequency (f_d = 36 ± 2 Hz) in the upward-facing orientation were independent of δ_(MPC). The active nucleation site densities on MPC, based on these values of D_d and f_d and the boiling curves in the experiments, ranged from ~725 to 1.07 × 10~4 sites/cm~2.
机译:PF-5060电介质在接近大气压(〜0.085 MPa)的微孔铜(MPC)上进行的饱和池沸腾实验研究了倾角(θ)和厚度(δ_(MPC))对成核沸腾(NB)的影响)传热系数(h_(NB))和临界热通量(CHF)。在实验中,δ_(MPC)在80到230μm之间变化,θ在0°(朝上)到180°(朝下)之间变化。除了增强h_(NB),在沸腾开始之前,表面温度(<5 K)没有(或轻微)偏移。 δ_(MPC)从95μm增加到230μm将CHF从22 W / cm〜2增加到26 W / cm〜2。完全发展的NB区末端附近的最高[最大核沸腾(MNB)]传热系数(h_(MNB))发生在比CHF更低的过热处。 h_(NB)和h_(MNB)均随δ_(MPC)的增加而增加,在〜171μm处达到峰值,然后随δ_(MPC)的进一步增加而下降。它们在朝上方向上最高。 h_(MNB)值(约7.8 W / cm〜2•K)随着θ增大到90°而缓慢下降,然后迅速下降到180°的最低值。在朝上的方向上,h_(NB)与所施加的热通量相​​关(h_(NB)= Aq〜B);当δ_(MPC)从80增大到230μm时,系数A从0.427线性增加到1.143,而在δ_(MPC)〜162μm时B从0.522增大到0.686的峰值,然后在δ_(MPC)=减小到0.573 230微米h_(NB)相关性与数据吻合在±12%以内。还开发了在低热通量(<0.48 W / cm〜2)下MPC上瞬时气泡生长的相关性。使用摄像机以每秒210帧的速度记录的立足点的测量结果之间的相关性在±5%之内。气泡朝上的离开直径(D_d = 431±7μm)和脱离频率(f_d = 36±2 Hz)与δ_(MPC)无关。根据这些D_d和f_d值以及实验中的沸腾曲线,MPC上的活性成核位点密度范围为〜725至1.07×10〜4个位点/ cm〜2。

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