A cost-effective experimental investigation of flow noise with a small-scale buoyancy or ballast-driven model (BDM), aimed at obtaining accurate measurements of total radiated sound power from the model, is presented. Two BDMs, approximately 0.9 m in length, are considered, operating in the DSTG Large Water Tank, which has a length, width and depth of 10 m \(\times \) 10 m \(\times \) 6 m, respectively. The tank functions as a highly reverberant space, and standard room-acoustic methods are used to measure the total radiated power in fractional-octave bands based on the tank reverberation times. The BDMs can reach speeds of order 7 m/s within about 0.7 s, often close to terminal velocity in the case of a buoyant model, before breaching the surface or hitting the bottom. Radiated power estimates are corrected for the reverberant lag associated with non-constant velocity of the model. Radiated noise following the expected sixth power of velocity is observed in the measurements. CFD modelling using the BDM shape, video-based dot-tracking measurements of the BDM motion, and internal accelerometer measurements, are combined to quantify the BDM characteristics such as added mass and drag coefficient, and thus the achievable terminal velocity.

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Study of Flow Noise with a Buoyancy-Driven Model

  • Ian MacGillivray,
  • Daniel Lamos,
  • Jeffrey Seers,
  • Alex Skvortsov

摘要

A cost-effective experimental investigation of flow noise with a small-scale buoyancy or ballast-driven model (BDM), aimed at obtaining accurate measurements of total radiated sound power from the model, is presented. Two BDMs, approximately 0.9 m in length, are considered, operating in the DSTG Large Water Tank, which has a length, width and depth of 10 m \(\times \) 10 m \(\times \) 6 m, respectively. The tank functions as a highly reverberant space, and standard room-acoustic methods are used to measure the total radiated power in fractional-octave bands based on the tank reverberation times. The BDMs can reach speeds of order 7 m/s within about 0.7 s, often close to terminal velocity in the case of a buoyant model, before breaching the surface or hitting the bottom. Radiated power estimates are corrected for the reverberant lag associated with non-constant velocity of the model. Radiated noise following the expected sixth power of velocity is observed in the measurements. CFD modelling using the BDM shape, video-based dot-tracking measurements of the BDM motion, and internal accelerometer measurements, are combined to quantify the BDM characteristics such as added mass and drag coefficient, and thus the achievable terminal velocity.