| 1. | Second order phase change
二级相变 |
| 2. | Situation of 2nd - order phase transition rigidization technique used in space inflatable structure
空间充气展开结构二级相变硬化技术研究现状 |
| 3. | Based on our dynamical study the liquid - gas phase transition in nuclei seems to be the second order phase transition
45左右。所有的上述的分析，还一致的给出了原子核的液气相变为二级相变。 |
| 4. | The position of the second order phase transition points for the stationary black holes has been argued by many authors recently
稳态黑洞在什么条件下出现二级相变，近年来在引力学界存在着争论。 |
| 5. | Then we expatiate on the methods of investigating phase transition , in particularly , and expound the theories of equilibrium and non - equilibrium fluctuations
在第二章中我们介绍了研究稳态黑洞二级相变的主要方法，其中重点阐述了系统的平衡涨落和非平衡涨落方法。 |
| 6. | In this paper , making use of both the thermodynamical equilibrium and the non - equilibrium fluctuations , we ascertain the position of the second order phase transition points in the stationary black holes , and discuss their physic meanings
本文采用平衡涨落和非平衡涨落两种方法对此进行了深入的研究，我们发现黑洞二级相变点的具体位置与研究中所采用的方法无关。 |
| 7. | We first introduce the second order phase transition theory in the general thermodynamical system , and make a brief summary of the about investigations of the second order phase transitions in stationary black holes in the recent years
在第一章中，我们首先介绍一般热力学系统的二级相变理论，描述了相变的一些主要特征。然后简单地回顾了黑洞热力学中的一些基本概念以及近年来对黑洞二级相变的一些研究状况。 |
| 8. | In summary , whether making use of the thermodynamical equilibrium fluctuations or the non - equilibrium fluctuations , we find that the second order phase transition points lie in where the heat capacities approach infinite , rather than where r + r _ in the stationary black holes
摘要h由以上讨论我们得到如下结论:无论是采用平衡涨落方法，还是采用非平衡涨落方法，稳态黑洞的二级相变点都位于热容量无穷大的地方 |
| 9. | At the phase transition points , both the thermodynamical equilibrium and non - equilibrium fluctuations in these black holes approach infinite ; ( 3 ) because both of the thermodynamical fluctuations in all stationary black holes listed above approach zero , the second order phase transitions dose n ' t occur when r + r _
此时，无论是在黑洞的平衡涨落中还是在非平衡涨落中，总有一些热力学量的涨落趋于无穷大。 ( 3 )它们在r _ + r _ -的地方没有发生二级相变。此时，黑洞所有的热力学涨落都变为0 。 |
| 10. | Some people draw a conclusion that the second order phase transition point in the stationary black hole lies in where the heat capacity tend to infinity by means of the thermodynamical equilibrium fluctuations . but the other people obtain a different conclusion that the second order phase transition takes place when r + - r - by using of the thermodynamical non - equilibrium fluctuations
一些学者利用平衡涨落的方法得出黑洞的二级相变点位于比热趋向于无穷大的地方；另一些学者采用非平衡涨落的方法则发现黑洞的二级相变点应位于其内、外视界相重叠的地方。 |
