Analysis Of Water Surface Oscillations Induced By Waves In The Pits Of The Intake Pipeline

K. Ishino
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Abstract

Technology Research Center, Taisei Corporation 344-1 Nasemachi Totukaku Yokohama 245, Japan The water intakes of plants near the coast facing the open sea may sometimes be affected by waves. When waves enter into the intake, free water surfaces in manholes, pump pits, etc., of the intake pipeline system are forced to move up and down. If the amplitude of oscillation increases, water may overflow manholes, or the suction of pumps may drop. Senshu et a1 (1969) studied theoretical analysis of forced oscillations of water surface in a pit of an intake pipeline due to waves. This paper describes the basic equations and numerical analysis procedure of forced oscillations of water surface in the pits of intake pipelines due to waves. The validity of numerical analysis procedure was confirmed by comparing the calculated amplitude of oscillations with the results of experiment. The calculated amplitude of oscillations agreed with the experiment results. INTRODUCTION Cooling water intakes are often located near the coast facing the open sea because plants near the coast commonly use seawater for cooling. In the pipeline between the cooling water intake and the pump room, pits (manholes) such as those for the entry of robots which remove marine life from the inner wall are often installed. When waves are incident on such a coastal intake pipelines, oscillations occur on the free water surface in the pits. Severe water surface oscillations may cause water to overflow from the pit, entrainment of air into the pump resulting in abnormally low water levels in the pump pit, or problems with the capacity of the pump (see Fig. 1 Conceptual Outline of Water Intake Facilities). To avoid such problems, the oscillations of each water surface must be calculated for waves incident on the intake. Analysis of free water surface oscillations in a water intake pipeline is found in Senshu's report. In Senshu's report, a pipeline with a single free water surface at the end of a one-way water intake pipe is considered. Pit (manhole) Pump pit Sea wall /----I\ Water over flow Side view Ld = 1 9 3 . 2 ~ ~ Fig. 2 Branch water intake model Branch water intakes and water intakes with several free surfaces were not studied. This paper describes a numerical analysis of forced water surface oscillations in the pits of intake pipelines due to waves. Secondly, the results of a hydraulic model experiment which was undertaken to verify the analysis are presented. WATER SURFACE OSCILLATION ANALYSIS 1. Basic equations for water surface oscillation The continuity equations and equations of motion are given below for the water flow between the free water surfaces of the branch water intake pipelines shown in Fig. 2 1.1 Equations of continuity AI-dZl . -al*Vl+a2*V2 ..................... (1) d t dz2 d z 3 A2'= -a2-V2+a3-V3+a4*V4 ............... (2) A3.= -a3*V3 ............................ (3) d t d t d z 4 A4'= -a4*V4 ........................... (4) d t The t h i r d term on the right-hand side of eq. (2) denotes "branch" . 1.2 Equations of motion dV1 z1-po/w-clI VI I * V I (5) .................. d t Ll/g dV3 23-22-C3' 1 V3 I ' V 3 .................... ( 7 ) = d t L 3 / s Fig. 1 Conceptual Outline of the Water Intake Facilities 1567
进气管道坑内波浪引起的水面振荡分析
日本,横滨面向大海的靠近海岸的工厂的取水量有时可能会受到海浪的影响。当波浪进入进水口时,进水口管道系统的人孔、泵坑等处的自由水面被迫上下移动。如果振荡幅度增大,水可能溢出人孔,或者泵的吸力可能下降。Senshu et a1(1969)研究了波浪作用下进气管道坑内水面强迫振荡的理论分析。本文介绍了波浪作用下进水管坑内水面强迫振荡的基本方程和数值分析方法。将计算得到的振动幅值与实验结果进行比较,验证了数值分析方法的有效性。计算得到的振动幅值与实验结果吻合。冷却水入口通常位于靠近海岸面朝大海的地方,因为靠近海岸的工厂通常使用海水进行冷却。在冷却水进水口和泵房之间的管道中,通常会安装凹坑(人孔),例如用于机器人进入的凹坑(人孔),这些凹坑用于从内壁清除海洋生物。当波浪入射到这样的海岸进气管道上时,在坑内的自由水面上发生振荡。严重的水面振荡可能导致水从坑中溢出,空气被吸入泵内,导致泵坑内水位异常低,或泵的容量出现问题(见图1取水设施概念概要)。为了避免这样的问题,必须计算入射到进水口的波浪在每个水面上的振荡。Senshu的报告中发现了取水管道中自由水面振荡的分析。在Senshu的报告中,考虑了单向进水管末端具有单一自由水面的管道。坑(人孔)泵坑海堤/----I\水流侧视图Ld = 1 9 3。2 ~ ~图2支路取水模型支路取水和多个自由面取水未进行研究。本文对波浪作用下进气管道坑内受迫水面振荡进行了数值分析。其次,给出了验证分析的水力模型试验结果。水面振荡分析图2所示分支取水管道自由水面间水流的连续性方程和运动方程如下:1.1连续性方程AI-dZl。过程*六世+ a2 * V2 .....................(1) 3 d t时d z A2 ' = A2 v2 + a3-V3 V4 + a4 * ...............(2) A3。= -a3*V3 ............................(3) z d t d t d 4 A4 ' = A4 * V4 ...........................式(2)右侧的th r d项表示“分支”。1.2运动方程dV1 z1-po / w-clI VI我(5 * V ) ..................d t会/ g dV3 23-22-C3 1 V3的V 3 ....................图1取水设施概念轮廓图
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