On the Distribution of the First-Passage Time for Normal Stationary Random Processes
On the Distribution of the First-Passage Time for Normal Stationary Random Processes
复制标题
DOI:
10.1115/1.3423521
复制
发表时间:
1975-03
期刊:
影响因子:
--
通讯作者:
E. Vanmarcke
中科院分区:
文献类型:
--
作者:
E. Vanmarcke
A quantity of central interest in many applications of the theory of stochastic processes to the analysis and design of engineering systems is the probability that a random motion X (t) will be kept within prescribed bounds during the system operating time, or the probability distribution of the time to first passage across specified barriers. Attention is restricted herein to stationary Gaussian processes with zero mean value and three barrier configurations are considered, as in Crandall, et al.[I]. 1 The first configuration involves a single barrier, X (t)= a, where a is a critical level not to be surpassed. In the second, the bounds consist of a pair of lines, X (t)= a and X (t)=—a, and the safe region is defined by| Xft)|< a. The third barrier, R (t)= a, which is defined in terms of the envelope R (t) of the random process X (t), is considered principally because it leads to useful approximations to the first-passage probability for single and double barriers. The envelope definition used is that of Cramer and Leadbetter [2] which is essentially equivalent to that of Rice [3]. The three barrier configurations are subsequently referred to as type-B, type-D, and type-£ barriers, respectively, and the excursions into the unsafe domain are called B-crossings, D-crossings and E-crossings, respectively [1].