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A 2D fast near-field method for calculating near-field pressures generated by apodized rectangular pistons

机译:二维快速近场方法,用于计算变迹矩形活塞产生的近场压力

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摘要

Analytical two-dimensional (2D) integral expressions are derived for fast calculations of time-harmonic and transient near-field pressures generated by apodized rectangular pistons. These 2D expressions represent an extension of the fast near-field method (FNM) for uniformly excited pistons. After subdividing the rectangular piston into smaller rectangles, the pressure produced by each of the smaller rectangles is calculated using the uniformly excited FNM expression for a rectangular piston, and the total pressure generated by an apodized rectangular piston is the superposition of the pressures produced by all of the subdivided rectangles. By exchanging summation variables and performing integration by parts, a 2D apodized FNM expression is obtained, and the resulting expression eliminates the numerical singularities that are otherwise present in numerical models of pressure fields generated by apodized rectangular pistons. A simplified time space decomposition method is also described, and this method further reduces the computation time for transient pressure fields. The results are compared with the Rayleigh–Sommerfeld integral and the FIELD II program for a rectangular source with each side equal to four wavelengths. For time-harmonic calculations with a 0.1 normalized root mean square error (NRMSE), the apodized FNM is 4.14 times faster than the Rayleigh–Sommerfeld integral and 59.43 times faster than the FIELD II program, and for a 0.01 NRMSE, the apodized FNM is 12.50 times faster than the Rayleigh–Sommerfeld integral and 155.06 times faster than the FIELD II program. For transient calculations with a 0.1 NRMSE, the apodized FNM is 2.31 times faster than the Rayleigh–Sommerfeld integral and 4.66 times faster than the FIELD II program, and for a 0.01 NRMSE, the apodized FNM is 11.90 times faster than the Rayleigh–Sommerfeld integral and 24.04 times faster than the FIELD II program. Thus, the 2D apodized FNM is ideal for fast pressure calculations and for accurate reference calculations in the near-field region.
机译:解析二维(2D)积分表达式用于快速计算由切趾矩形活塞产生的时谐和瞬态近场压力。这些2D表达式代表了均匀激励活塞的快速近场方法(FNM)的扩展。将矩形活塞细分为较小的矩形后,使用矩形活塞的均匀激发的FNM表达式计算每个较小的矩形所产生的压力,并且切趾矩形活塞所产生的总压力是所有活塞所产生的压力的叠加细分的矩形。通过交换求和变量并按部分进行积分,可以获得二维切趾的FNM表达式,并且所得表达式消除了由切趾的矩形活塞生成的压力场的数值模型中不存在的数值奇点。还描述了一种简化的时空分解方法,该方法进一步减少了瞬态压力场的计算时间。将结果与Rayleigh-Sommerfeld积分和FIELD II程序进行比较,对于矩形光源,每边等于四个波长。对于具有0.1归一化均方根误差(NRMSE)的时谐计算,切趾的FNM比Rayleigh–Sommerfeld积分快4.14倍,比FIELD II程序快59.43倍;对于0.01 NRMSE,切趾的FNM为比Rayleigh-Sommerfeld积分快12.50倍,比FIELD II程序快155.06倍。对于使用0.1 NRMSE的瞬态计算,切趾的FNM比Rayleigh–Sommerfeld积分快2.31倍,比FIELD II程序快4.66倍;对于0.01 NRMSE,切趾的FNM比Rayleigh–Sommerfeld积分快11.90倍并且比FIELD II程序快24.04倍。因此,二维切趾的FNM是快速压力计算和近场区域精确参考计算的理想选择。

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