Reducing contaminating noise effects when calculating low-boom loudness levels

  • 0Department of Physics and Astronomy, Brigham Young University, Provo, Utah 84602, USA.

Summary

This summary is machine-generated.

NASA

Area Of Science

  • Acoustics
  • Aerospace Engineering
  • Signal Processing

Background

  • Low-boom supersonic aircraft like NASA's X-59 generate sonic booms that can be perceived differently due to noise contamination.
  • Instrumentation and ambient noise can inflate sonic boom perception metrics by several decibels, affecting test accuracy.

Purpose Of The Study

  • To develop and compare robust low-pass filtering techniques for removing noise contamination from low-boom recordings.
  • To assess the effectiveness of these filters in improving the accuracy of sonic boom perception metrics.

Main Methods

  • Development and application of a time-domain Butterworth-magnitude filter.
  • Development and application of a frequency-domain Brick Wall filter.
  • Comparison of filter performance against simulated and real-world noise data and a modified ISO 11204 correction.

Main Results

  • Both the Butterworth and Brick Wall filters effectively reduced noise contamination in metric calculations.
  • The filters demonstrated comparable performance to the modified ISO 11204 correction.
  • The Butterworth filter successfully removed statistical correlation between ambient and boom levels in real-world data.

Conclusions

  • Robust low-pass filtering techniques, specifically Butterworth and Brick Wall filters, can accurately calculate sonic boom metrics even with moderate noise contamination.
  • These methods are beneficial for NASA's X-59 and future low-boom supersonic aircraft testing, ensuring reliable data collection.

Related Concept Videos

Sound Intensity Level 00:53

4.2K

Humans perceive sound by hearing. The human ear helps sound waves reach the brain, which then interprets the waves and creates the perception of hearing. The loudness of the environment in which a person is located determines whether they can distinguish between different sound sources.
The human ear can perceive an extensive range of sound intensity, necessitating the use of the logarithmic scale to define a physical quantity—the intensity level. It is a ratio of two intensities and...

Shock Waves 01:16

2.0K

While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high...

Sound Waves: Interference 00:53

3.7K

Sound waves can be modeled either as longitudinal waves, wherein the molecules of the medium oscillate around an equilibrium position, or as pressure waves. When two identical waves from the same source superimpose on each other, the combination of two crests or two troughs results in amplitude reinforcement known as constructive interference. If two identical waves, that are initially in phase, become out of phase because of different path lengths, the combination of crests with troughs...

Sound Intensity 00:58

4.0K

The loudness of a sound source is related to how energetically the source is vibrating, consequently making the molecules of the propagation medium vibrate. To measure the loudness of a source, the physical quantity of interest is the intensity. This is defined as the energy emitted per unit of time per unit of area perpendicular to the sound wave's propagation direction. Since the total energy is greater if the source vibrates for a longer duration and over a larger area, dividing the...

Upsampling 01:22

225

Managing signal sampling rates is essential in digital signal processing to maintain signal integrity. A decimated signal, characterized by a reduced frequency range due to its lower sampling rate, can be upsampled by inserting zeros between each sample. This upsampling process expands the original spectrum and introduces repeated spectral replicas at intervals dictated by the new Nyquist frequency. To refine this zero-inserted sequence, it is passed through a lowpass filter with a cutoff...

Downsampling 01:20

149

When considering a sampled sequence with zero values between sampling instants, one can replace it by taking every N-th value of the sequence. At these integer multiples of N, the original and sampled sequences coincide. This process, known as decimation, involves extracting every N-th sample from a sequence, thereby creating a more efficient sequence.
The Fourier transform of the decimated sequence reveals a combination of scaled and shifted versions of the original spectrum. This...