軟孔隙彈性介質底床之流體動力反應

博士 === 國立臺灣大學 === 土木工程學研究所 === 87 === When oscillatory water wave propagating over a soft poroelastic bed, a boundary layer exists within the porous bed and near the homogeneous-water/porous-bed interface. Owing to the effect of boundary layer, the conventional evaluation of the second kind of long...

Full description

Bibliographic Details
Main Authors: PING-CHENG HSIEH, 謝平城
Other Authors: 黃良雄
Format: Others
Language:zh-TW
Published: 1999
Online Access:http://ndltd.ncl.edu.tw/handle/85850281091307524271
id ndltd-TW-087NTU00015016
record_format oai_dc
spelling ndltd-TW-087NTU000150162016-02-01T04:12:23Z http://ndltd.ncl.edu.tw/handle/85850281091307524271 軟孔隙彈性介質底床之流體動力反應 PING-CHENG HSIEH 謝平城 博士 國立臺灣大學 土木工程學研究所 87 When oscillatory water wave propagating over a soft poroelastic bed, a boundary layer exists within the porous bed and near the homogeneous-water/porous-bed interface. Owing to the effect of boundary layer, the conventional evaluation of the second kind of longitudinal wave inside the soft poroelastic bed by one parameter is very inaccurate so that a systematic boundary layer correction approach for soft poroelastic bed is proposed to solve the nonlinear water wave problem in the present study. After analyzing the length scale and order of magnitude of physical variables, perturbation expansion for the boundary layer correction approach based on two small parameters is proposed and then solved. The solutions which are carried out to the first three terms for suppressing secular phenomena are valid for the first kind and the third kind of waves throughout the whole domain. The second kind of wave is solved systematically inside the boundary layer while it disappears outside the boundary layer. This study successfully derives the complete governing equations and boundary conditions which especially inside the boundary layer for the second kind of wave are built to overcome the difficulty that Chen, Huang & Song(1997) met. The linear water wave solution is compared with the result of Huang & Song (1993) in order to verify the validity of the present approach. Based on the analysis of linear solution, a simplified boundary value formulation, which is expected to be very useful in numerical computation, is also proposed by decomposing the physical variables into in-phase and out-of-phase parts. Shi (1998) adopted this concept to improve the execution of numerical computation as well as save much CPU time and then got satisfactory results. Then the nonlinear water wave solution is proposed to improve the result of Chen, Huang & Song(1997) who failed to estimate the second kind of wave accurately. Moreover, when considering current effect, the solutions obtained by Runge-Kutta method can be traced automatically to different flow regime of bed forms including dune, antidune and flat bed, which improve Chiang’s (1994) results much better without the discontinuous phenomena and artificial judgement. In addition, an approximate criterion of soil liquefaction at the surface of soft poroelastic bed is proposed and the liquefaction phenomena are also observed. 黃良雄 王燦汶 1999 學位論文 ; thesis 178 zh-TW
collection NDLTD
language zh-TW
format Others
sources NDLTD
description 博士 === 國立臺灣大學 === 土木工程學研究所 === 87 === When oscillatory water wave propagating over a soft poroelastic bed, a boundary layer exists within the porous bed and near the homogeneous-water/porous-bed interface. Owing to the effect of boundary layer, the conventional evaluation of the second kind of longitudinal wave inside the soft poroelastic bed by one parameter is very inaccurate so that a systematic boundary layer correction approach for soft poroelastic bed is proposed to solve the nonlinear water wave problem in the present study. After analyzing the length scale and order of magnitude of physical variables, perturbation expansion for the boundary layer correction approach based on two small parameters is proposed and then solved. The solutions which are carried out to the first three terms for suppressing secular phenomena are valid for the first kind and the third kind of waves throughout the whole domain. The second kind of wave is solved systematically inside the boundary layer while it disappears outside the boundary layer. This study successfully derives the complete governing equations and boundary conditions which especially inside the boundary layer for the second kind of wave are built to overcome the difficulty that Chen, Huang & Song(1997) met. The linear water wave solution is compared with the result of Huang & Song (1993) in order to verify the validity of the present approach. Based on the analysis of linear solution, a simplified boundary value formulation, which is expected to be very useful in numerical computation, is also proposed by decomposing the physical variables into in-phase and out-of-phase parts. Shi (1998) adopted this concept to improve the execution of numerical computation as well as save much CPU time and then got satisfactory results. Then the nonlinear water wave solution is proposed to improve the result of Chen, Huang & Song(1997) who failed to estimate the second kind of wave accurately. Moreover, when considering current effect, the solutions obtained by Runge-Kutta method can be traced automatically to different flow regime of bed forms including dune, antidune and flat bed, which improve Chiang’s (1994) results much better without the discontinuous phenomena and artificial judgement. In addition, an approximate criterion of soil liquefaction at the surface of soft poroelastic bed is proposed and the liquefaction phenomena are also observed.
author2 黃良雄
author_facet 黃良雄
PING-CHENG HSIEH
謝平城
author PING-CHENG HSIEH
謝平城
spellingShingle PING-CHENG HSIEH
謝平城
軟孔隙彈性介質底床之流體動力反應
author_sort PING-CHENG HSIEH
title 軟孔隙彈性介質底床之流體動力反應
title_short 軟孔隙彈性介質底床之流體動力反應
title_full 軟孔隙彈性介質底床之流體動力反應
title_fullStr 軟孔隙彈性介質底床之流體動力反應
title_full_unstemmed 軟孔隙彈性介質底床之流體動力反應
title_sort 軟孔隙彈性介質底床之流體動力反應
publishDate 1999
url http://ndltd.ncl.edu.tw/handle/85850281091307524271
work_keys_str_mv AT pingchenghsieh ruǎnkǒngxìdànxìngjièzhìdǐchuángzhīliútǐdònglìfǎnyīng
AT xièpíngchéng ruǎnkǒngxìdànxìngjièzhìdǐchuángzhīliútǐdònglìfǎnyīng
_version_ 1718173818121355264