浅谈粉煤灰路基的施工

在江汉平原,人均耕地面积较少,土地肥沃,取土进行路基填筑会减少大量的耕地。本标段充分利用陈年积压、占用大量良田的二期粉煤灰进行路基填筑,既还建了良田,又解决了环境污染。结合工程实际,介绍了先填筑粉煤灰再填筑包边土路基的施工方法。     

Two-dimensional numerical simulation and experiment on strongly nonlinear wave–body interactions

A constrained interpolation profile (CIP)-based Cartesian grid method for strongly nonlinear wave–body interaction problems is presented and validated by a newly designed experiment, which is performed in a two-dimensional wave channel. In the experiment, a floating body that has a rectangular section shape is used. A superstructure is installed on the deck and a small floating-body freeboard is adopted in order to easily obtain water-on-deck phenomena. A forced oscillation test in heave and a wave–body interaction test are carried out. The numerical simulation is performed by the CIP-based Cartesian grid method, which is described in this paper. The CIP scheme is applied in the Cartesian grid-based flow solver. New improvements of the method include an interface-capturing method that applies the tangent of hyperbola for interface capturing (THINC) scheme and a virtual particle method for the floating body. The efficiency of the THINC scheme is shown by a dam-breaking computation. Numerical simulations on the experimental problem for both the forced oscillation test and the wave–body interaction test are carried out, and the results are compared to the measurements. All of the comparisons are reasonably good. It is shown, based on the numerical examples, that the present CIP-based Cartesian grid method is an accurate and efficient method for predicting strongly nonlinear wave–body interactions.     

Database of sail shapes versus sail performance and validation of numerical calculations for the upwind condition

A database of full-scale three-dimensional sail shapes is presented with the aerodynamic coefficients for the upwind condition of International Measurement System (IMS) type sails. Three-dimensional shape data are used for the input of numerical calculations and the results are compared with the measured sail performance. The sail shapes and performance were measured using sail dynamometer boat Fujin. This is a boat of 10.3-m length overall in which load cells and CCD cameras were installed to simultaneously measure the sail forces and shapes. At the same time, the sailing conditions of the boat, e.g., boat speed, heel angle, wind speed, and wind angle, were measured. The sail configurations tested were: mainsail with 130% jib, mainsail with 75% jib, and mainsail alone. Sail shapes were measured at several vertical positions for the shape parameters defined by: chord length, maximum draft, maximum draft position, entry angle at the luff, and exit angle at the leech, all of which finally yield three-dimensional coordinates of the sail geometry. The tabulated shape data, along with aerodynamic coefficients, are presented in this article. In addition, numerical flow simulations were performed for the measured sail shapes and the sailing conditions to investigate the capability and limitations of the methods through detailed comparison with the measurements. Two numerical methods were used: a vortex lattice method (VLM) and a Reynolds-averaged Navier–Stokes (RANS)-based computational fluid dynamics method. The sail shape database, in association with the numerical results, provides a good benchmark for the sail performance analysis of the upwind condition of IMS type sails.     

Unsteady finite-depth effects during resistance tests on a ship model in a towing tank

This paper covers an extension of the study of Doctors et al. (J Ship Res 52(4):263–273, 2008) on oscillations in wave resistance during the constant-velocity phase of a towing-tank resistance test on a ship model to the case of relatively shallow water. We demonstrate here that the unsteady effects are very prominent and that it is essentially impossible to achieve a steady-state resistance curve in a towing tank of typical proportions for a water-depth-to-model-length ratio of 0.25. This statement is particularly true in the speed region near a depth Froude number of unity. However, on the positive side, we show here that an application of unsteady linearized wave-resistance theory provides an excellent prediction of the measured total resistance, when one accounts for the form factor in the usual manner. Finally, a simple application of the results to the planning and analysis of towing-tank tests is presented.     

Water entry of a bow-flare ship section with roll angle

The two-dimensional water entry of a bow-flare ship section with constant roll angle, or heel angle, was studied by using a boundary element method. The fully nonlinear free surface conditions and exact body boundary conditions were satisfied. Nonviscous flow separation from the knuckles of the section or from the curved bottom could be simulated. The numerical calculations were compared with existing experimental results. First, the effects of roll angle were investigated and then the characteristics associated with large roll angles were examined in particular. The evolution of the free surfaces and the pressure distributions on the section surface are illustrated and the influence of nonviscous flow separation from the leeward section surface is discussed.     

海上溢油收集装置概念设计

随着海洋石油开采和运输事业的日益发展,海上溢油问题的研究越来越受到重视,具有重要的理论价值和实际意义.论文针对各类海上溢油事故,在现有技术的基础上进行突破和创新,提出了三套新概念的海上溢油处理装置,热气球海上浮油收集装置、海上铲车浮油收集器和下潜式浮油收集器,分别利用漩涡原理,面面接触的物理方式和生物环保技术,有效提高海上溢油的收集效率,丰富了溢油处理装置的设计理念,为后续的详细设计奠定了基础.     

3600t化学品船主推进系统安装工艺

为了更合理地进行3600t化学品船主推进系统设备的安装,对轴系采用负荷法校中,使轴系各轴承负荷分配更趋合理。编制安装工艺,指导和控制各设备的安装步序以及安装质量要求,使船厂缩短了安装周期,并且通过了船东、船检的认可和验收。     

LNG船疲劳强度评估及低温影响的讨论

以某LNG船为研究对象,建立三舱段有限元模型,并根据美国船级社薄膜型LNG船体结构疲劳强度指南,基于SN曲线法的疲劳积累损伤原理,分别采用名义应力和热点应力法,对船体典型节点进行疲劳强度评估,同时对计算结果进行分析;讨论低温下材料性能改变对节点疲劳寿命评估的影响。研究表明,采用常温下SN曲线进行LNG船疲劳强度评估是合适的。     

运输船电力负荷计算探讨

文章对电力负荷计算的计算方法、计算工况、设备本身功率的选取、计算表中涉及的相关系数的确定等四个方面的问题进行探讨,分别阐述了它们对电站配置的重要影响,并提出了合理配置电站的基本思考原则。     

大型集装箱船参数横摇模型试验和数值模拟研究

以4000TEU集装箱船为研究对象,通过系列自航模型试验,确定其在迎浪规则波中发生参数横摇的限界。试验结果显示：在迎浪规则波中,参数横摇通常发生在波浪遭遇周期为横摇固有周期一半的附近;对应不同遭遇频率时参数横摇的发生,存在一个临界波高;航速的增加和舭龙骨的安装将使参数横摇发生的临界波高增加;当有初始干扰时,参数横摇发生的临界波高较小。而且,数值模拟结果与模型试验结果比较吻合。