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温度不均匀分布

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According to the experimental data, it is found that the circumferential diffierence of heat transfer characteristics occurres due to the effects of thermal acceleration and buoyance in the inclined smooth tube at supercritical pressure.

实验结果表明:在超临界压力区域,倾斜光管内可能由于受到热加速度和浮力的综合作用,倾斜光管传热特性沿周向是不均匀分布状态,通常管内顶部的壁面温度比底部高,在大比热区发生传热恶化和传热强化的现象,低质量流速和高热负荷条件下会发生传热恶化现象,高质量流速下会发生传热强化,避免壁温发生飞升;内螺纹管内的传热特性在不同焓值区域表现不同,在远离拟临界焓值的低焓值区域和高焓值区域,呈现出相似的规律,而在接近拟临界焓值区域时,传热得到强化。

Because of the uneven temperature's distribution in the space,the detected temperature'value will vary with the different placement of the temperature sensor in detecting temperature and then need to know the distributing curve of temperature in the given space.

由于温度在空间中分布不均匀,在进行温度检测时会出现检出温度随着温度传感器放置位置的不同而不同的现象,这时就需要知道特定空间内的温度分布曲线。

The results indicate that the flow stress of the alloy increases with increasing strain rate and decreasing deformation temperature. The flow stress increases with increasing strain until the stress reaches the peak value, then the flow stress remains constant, which indicates that dynamic recrystallization happens during deformation. The flow behaviors are described by the hyperbolic sine constitutive equation, and the activation energy calculated is 337.75 kJ/mol. The as-forged microstructure consists of refined α2/γ and γ grains, and the grains are much homogeneous than before. The B2 phase distributes uniformly at the grain boundary of α2/γ and γ grains. The B2 phase decreases with increasing deformation temperature.

结果表明:流变应力随着应变速率提高和变形温度降低而增大;在变形过程中,流变应力随着变形量增大而增大,当流变应力达到峰值后趋于平稳,表明合金在变形过程中发生了动态再结晶;热变形过程的流变应力可采用双曲正弦本构关系来描述,平均激活能为337.75 kJ/mol;从合金的组织演化过程中可以看出,合金中不均匀的原始组织得到明显均匀化,变形后的组织是由α2/γ层片晶团和γ晶粒组成的双态组织,在α2/γ层片晶团和γ晶粒的晶界交界处发现分布均匀的B2相,并且随着变形温度升高B2相数量逐渐减少。

The results show that the temperature change of the heat exchanger is consistent with flow pattern and the maldistribution is more and more severe with the increase of Re velues.

实验结果表明随着Re的增大,换热器出口温度分布与流量分配趋势相一致,会越来越不均匀;较大的传热温差也会增加温度分布的不均匀性。

In addition, larger temperature difference of heat transfer can enlarge the maldistribution of the temperature.

通过比较二次封头和普通封头换热器截面温度分布情况发现:二次封头结构明显地改善了换热器出口截面温度分布,尤其在大Re下,温度分布不均匀性的改善效果更加显著,同时换热效能可增加7%左右。

Experimental research on indoor air temperature distributions with underfloor air supply .

地板送风室内温度不均匀分布特性的实验研究。

At first,the curve of charge distribution,ionizable state of nonisothermatity sphere,Was obtained by computer to calculate ionized state according to distribution data of temperature and dinsity within Earth. Secondly,the pussibility of microgravitational testonosphere,Within the isothermality sphere,was found by balance between pressure and volumetric forcein Earth's interior.The thickness is 1 000 km or so.Finally,the result come into commom use various geophysical process withi...

首先依据地球内部温度和密度不均匀分布数据,用计算机计算它的电离状态,得到非等温分层电离状态的电荷分布曲线;其次从地球内部存在的流体压力与两类体积力:重力和静电力的平衡方程讨论中,发现在某一等温层内可能存在微重力构造圈,其厚度约为1000km左右;最后在地学研究向整体化和深部化发展趋势下,预期这个结果将有助于理解地球深部发生的各种物理过程且与地震S波在核-幔之间层中消失观测事实相一致。

Numerical analysis of unit heat generation rate and thermal flux density is conducted. Results show that the chamber's boundary extermal thermal conduction is the primary factor that leads to temperature ununiformity distrubtion inside the chamber.

而单元生热率及热流密度的数值结果表明,腔体边界上的对外热传导是温度不均匀分布的主要原因。

The numerical results become visible and vivid with software TECPLOT. And the data is processed to get temperature coefficient of ununiformity, velocity coefficient ununiformity and air diffusion performance index.

求得工作区域的速度不均匀系数、温度不均匀系数以及空气分布特性指标,为车室内气流组织分布的优化设计提供依据。

The temperature gradient is larger in case ofussual half-zone model which has a uniform temperature distribution on the hot rod,andmodified half-zone model which has a non-uniform temperature distribution in the hotrod and negative radial temperature gradient near the axis of the hot rod.

模拟半浮区模型提出选择热传导系数与试验液体相当的材料作为热端棒材,使得热端内侧的轴向温度梯度接近于零。模拟半浮区模型的温度分布更接近于全浮区温度分布的一半。对于改型半浮区模型,选择热传导系数高于试验液体值一个数量级的材料作为热端棒材,使得热端温度分布不均匀,并且热端内侧温度高于外侧温度。

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