Numerical study on aerodynamic noises and characteristics of the high-speed train in the open air and tunnel environment

When high-speed trains were passing through a tunnel, pressure wave will change seriously and cause large aerodynamic loads, which may bring problems to the comfort of passengers and the aerodynamic fatigue failure of train bodies, components and fixed equipment in the tunnel. Therefore, this paper systematically studied aerodynamic characteristics of a high-speed train under three kinds of situation including open air, entering a tunnel and completely in a tunnel, experimentally verified the correctness of numerically computational model. In the open air, vortexes of the high-speed train were mainly distributed in the bogie and compartment connections. Sound pressure level curves had many peak and valley points and the maximum sound pressure level was 72 dB. Sound pressure levels gradually decreased with the increase of analyzed frequency. In addition, sound energy was mainly distributed below 2000 Hz. Aerodynamic noises presented an obvious directivity and attenuation distribution. In the entering the tunnel, peak and valley values of pressures at train head and tail appeared at different time. The maximum pressures at the observation points of train head and tail were 345 Pa and –450 Pa respectively, while the minimum negative pressures at the observation points of train head and tail were –2900 Pa and –3260 Pa respectively. Computational pressures of observation points were basically consistent with the experimental test, and the relative error was only within 2 %, which indicated that the adopted numerical simulation can better simulate aerodynamic characteristics of the high-speed train. The change of the length of the tunnel had no an obvious effect on the aerodynamic lift of the high-speed train. When the length of the tunnel was less than 800 m, the negative peak of the aerodynamic lift increased continuously with the extension of the tunnel, but the increased rate was gradually reduced. When the length of the tunnel was more than 800 m, the negative peak of the aerodynamic lift was gradually reduced. According to the acoustic panel contribution, these panels which had an obvious effect on the interior noise of the high-speed train were recognized. Composite sound absorption material was then applied to these panels and the interior noise at the observation points was improved obviously.

[1]  Jie Zhang,et al.  Effect of increased linings on micro-pressure waves in a high-speed railway tunnel , 2016 .

[2]  Aigen Huang,et al.  Semi-active control of piezoelectric coating׳s underwater sound absorption by combining design of the shunt impedances , 2015 .

[3]  J. Ih,et al.  On the reconstruction of the vibro‐acoustic field over the surface enclosing an interior space using the boundary element method , 1996 .

[4]  Di Zhang,et al.  Microstructure and sound absorption of porous copper prepared by resin curing and foaming method , 2015 .

[5]  Zhang Jian Influence of shaft on alleviating transient pressure in tunnel , 2011 .

[6]  Wang Ruili,et al.  Numerical Study on the Basic Characteristics of Pressure Waves at the Entrances of High Speed Railway Tunnels , 2016 .

[7]  Javier Cubas,et al.  On the Analytical Approach to Present Engineering Problems: Photovoltaic Systems Behavior, Wind Speed Sensors Performance, and High-Speed Train Pressure Wave Effects in Tunnels , 2015 .

[8]  P. Monkewitz,et al.  Comparison of mean flow similarity laws in zero pressure gradient turbulent boundary layers , 2008 .

[9]  Mathias Basner,et al.  Pressure variations on a train - Where is the threshold to railway passenger discomfort? , 2013, Applied ergonomics.

[10]  Luo Jianju Pressure change from the cross aisle when the train passing through parallel tunnel of high-speed railway , 2015 .

[11]  Javier García,et al.  Genetically aerodynamic optimization of the nose shape of a high-speed train entering a tunnel , 2014 .

[12]  Peter Keith Woodward,et al.  Optimising low acoustic impedance back-fill material wave barrier dimensions to shield structures from ground borne high speed rail vibrations , 2013 .

[13]  Yong Li,et al.  Unidirectional acoustic transmission through a prism with near-zero refractive index , 2013 .

[14]  S. Marburg,et al.  Computational acoustics of noise propagation in fluids : finite and boudary element methods , 2008 .

[15]  Kyu-Hong Kim,et al.  Effects of nose shape and tunnel cross-sectional area on aerodynamic drag of train traveling in tunnels , 2014 .

[16]  Hyo-gyu Kim,et al.  A comparative study of field measurements of the pressure wave with analytical aerodynamic model for the high speed train in tunnels , 2015 .

[17]  Chen Xiao-l Application of the mesh fusion method in numerical simulation of a high-speed train passing through a tunnel , 2016 .

[18]  Mingzhi Yang,et al.  A new calculation method for micro-pressure waves induced by high-speed train passing through long tunnels and bend tunnels , 2015 .

[19]  Preprint Mps Condition Number Estimates for Combined Potential Integral Operators in Acoustics and their Boundary Element Discretisation , 2010 .

[20]  K. Chang,et al.  Flow Similarity in Compressible Convex-Corner Flows , 2012 .

[21]  Ramani Duraiswami,et al.  Computation of the head-related transfer function via the fast multipole accelerated boundary element method and its spherical harmonic representation. , 2010, The Journal of the Acoustical Society of America.

[22]  T. Arai,et al.  Nondimensional maximum pressure gradient of tunnel compression waves generated by offset running axisymmetric trains , 2016 .

[23]  Jun Yang,et al.  Experimental study of the effect of viscoelastic damping materials on noise and vibration reduction within railway vehicles , 2009 .

[24]  Guan Yongjiu Investigation of Air Pressure Pulse When Two High-speed Trains Passing by Each Other in Tunnel , 2012 .

[25]  Tokuzo Miyachi,et al.  Acoustic model of micro-pressure wave emission from a high-speed train tunnel , 2017 .