首页> 外文会议>ASME/JSME Thermal Engineering Joint Conference >EFFECT OF THE BEHAVIOR OF GENERATED VAPOR ON THE MINIMUM-HEAT-FLUX POINT DURING RAPID QUENCHING OF A THIN HORIZONTAL WIRE
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EFFECT OF THE BEHAVIOR OF GENERATED VAPOR ON THE MINIMUM-HEAT-FLUX POINT DURING RAPID QUENCHING OF A THIN HORIZONTAL WIRE

机译:产生蒸汽的行为对薄水平线快速淬火期间最小热通量点的影响

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Heat transfer characteristics and minimum-heat-flux point (MHF point) condition during rapid quenching of a thin horizontal wire were studied both experimentally and theoretically. Experiments were conducted with ethanol as a quenching liquid. The wire was either fixed or moving downward at a constant speed in the ethanol bath. When the wire was heated instantaneously to a high temperature, the generated vapor formed bead-like bubbles along the wire as shown in Fig. A-1. This was in contrast to the previous results (Honda et al., 1995) for a heated wire that was dipped into the ethanol bath at a relatively high velocity, where a vapor sheet was formed in the wake of the wire. Consideration was given to the effect of the film boiling mode on the MHF point condition. A linear stability analysis of a vapor film for natural convection film boiling on a horizontal cylinder was presented that considered the effects of liquid inertia, viscosity and compressibility of vapor, and periodic heat transfer. Figure A-2 shows a comparison of the average vapor film thickness at the MHF point δ{sub}(MHF), the modified vapor film thickness at the MHF point based on the effective surface area (thin film region between bead-like bubbles) δ{sub}(MHF,M) and the theoretical prediction of the critical vapor film thickness δ{sub}(cr). It is seen from Fig. A-2 that δ{sub}(MHF) is smaller for higher liquid subcooling ΔT{sub}(sub). The δ{sub}(MHF,M) is not affected by ΔT{sub}(sub) and it increases gradually with increasing wall superheat ΔT{sub}(sat). It is also seen that δ{sub}(cr) compares well with δ{sub}(MHF,M).
机译:热传导特性和薄水平金属丝的快速淬火时的最小热通量点(MHF点)的条件下进行了实验和理论研究两者。实验用乙醇作为骤冷液中进行。将导线或者是固定的或者在乙醇浴中以恒定的速度向下移动。当线被瞬间加热到高温,如示于图A-1所形成的所产生的蒸汽珠状沿导线气泡。这是在对于被以相对高的速度,其中,形成于金属丝的唤醒的蒸气片浸入乙醇浴中加热的金属丝与先前的结果(Honda等人,1995)。考虑了薄膜沸腾模式对MHF点条件的影响。提出所考虑的液体惯性,粘性和蒸气的压缩性,和周期性传热的效果为在水平气缸自然对流薄膜沸腾蒸汽膜的线性稳定性分析。图A-2示出了在MHF点δ{子}(MHF)的平均蒸汽膜厚度的比较,以基于有效表面积的MHF点修饰的蒸汽膜厚度(珠状的气泡之间的薄膜区域) δ{子}(MHF,M)和临界蒸汽膜厚度δ{子}(CR)的理论预测。从图。A-2看出,δ{子}(MHF)可以较高液体过冷ΔT{子}(分)小。的δ{子}(MHF,M)不受ΔT{子}(分),并将它与增加壁过热ΔT{子}逐渐增大(饱和)。它也可以看出,δ{子}(CR)与δ{子}(MHF,M)进行比较好。

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