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. 2023 Jan 20;20(3):1955.
doi: 10.3390/ijerph20031955.

Integrated Evaluation of the Aeroacoustics and Psychoacoustics of a Single Propeller

Affiliations

Integrated Evaluation of the Aeroacoustics and Psychoacoustics of a Single Propeller

Jianwei Sun et al. Int J Environ Res Public Health. .

Abstract

Aeroacoustic noise in multiple rotor drones has been increasingly recognized as a crucial issue, while noise reduction is normally associated with a trade-off between aerodynamic performance and sound suppression as well as sound quality improvement. Here, we propose an integrated methodology to evaluate both aeroacoustics and psychoacoustics of a single propeller. For a loop-type propeller, an experimental investigation was conducted in association with its aerodynamic and acoustic characteristics via a hover stand test in an anechoic chamber; the psychoacoustic performance was then examined with psychoacoustic annoyance models to evaluate five psychoacoustic metrics comprising loudness, fluctuation strength, roughness, sharpness, and tonality. A comparison of the figure of merit (FM), the overall sound pressure level (OASPL) and psychoacoustic metrics was undertaken among a two-blade propeller, a four-blade propeller, the loop-type propeller, a wide chord loop-type propeller, and a DJI Phantom III propeller, indicating that the loop-type propeller enables a remarkable reduction in OASPL and a noticeable improvement in sound quality while achieving comparable aerodynamic performance. Furthermore, the psychoacoustic analysis demonstrates that the loop-type propeller can improve the psychological response to various noises in terms of the higher-level broadband and lower-level tonal noise components. It is thus verified that the integrated evaluation methodology of aeroacoustics and psychoacoustics can be a useful tool in the design of low-noise propellers in association with multirotor drones.

Keywords: aerodynamic noise; broadband noise; loop-type propeller; psychoacoustic; tonal noise.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Figure 1
Figure 1
The hover stand setup in an anechoic chamber for aerodynamic and acoustic measurements.
Figure 2
Figure 2
Five propellers: (a) two-blade propeller (#1), (b) four-blade propeller (#2), (c) loop-type propeller (#3), (d) wide chord loop-type propeller (#4), and (e) DJI Phantom propeller (#5).
Figure 3
Figure 3
Radial distributions of chord length (a) and pitch angle (b) of five propellers.
Figure 4
Figure 4
Comparison of (a) the thrust coefficient (Ct), (b) torque coefficient (CQ), and (c) figure of merit (FM) among the two-blade propeller (#1), four-blade propeller (#2), loop-type propeller (#3), wide chord loop-type propeller (#4), and DJI Phantom III propeller (#5).
Figure 5
Figure 5
Comparison of mechanical power vs. thrust at four stable thrusts of five propellers.
Figure 6
Figure 6
Comparison of the power spectral density of background noise, unloaded motor noise, and DJI Phantom III propeller (#5) (5400 RPM, θ=25 deg).
Figure 7
Figure 7
Power spectral density of five propellers at a rotational speed of 5400 RPM at Mic 2. (a) 100–20 kHz, (b) 100–4 kHz, and (c) 4.5–10 kHz.
Figure 7
Figure 7
Power spectral density of five propellers at a rotational speed of 5400 RPM at Mic 2. (a) 100–20 kHz, (b) 100–4 kHz, and (c) 4.5–10 kHz.
Figure 8
Figure 8
Comparison of OASPL among the two-blade propeller (#1), four-blade propeller (#2), loop-type propeller (#3), wide chord loop-type propeller (#4), and DJI Phantom III propeller (#5) at a rotational speed of 5400 rpm (a) and at a stable thrust of 3 N (b).
Figure 9
Figure 9
Contour maps of the SPL in dB (Mic 2, θ=25 deg) over a frequency range of 50–2000 Hz associated with propeller noises: (a) two-blade propeller (#1), (b) four-blade propeller (#2), (c) loop-type propeller (#3), (d) wide chord loop-type propeller (#4), and (e) DJI Phantom propeller (#5) at various rotational speeds.
Figure 9
Figure 9
Contour maps of the SPL in dB (Mic 2, θ=25 deg) over a frequency range of 50–2000 Hz associated with propeller noises: (a) two-blade propeller (#1), (b) four-blade propeller (#2), (c) loop-type propeller (#3), (d) wide chord loop-type propeller (#4), and (e) DJI Phantom propeller (#5) at various rotational speeds.
Figure 10
Figure 10
Contour maps of the SPL in dB (Mic 2, θ=25 deg) over a frequency range of 6000–10,000 Hz associated with propeller noises: (a) two-blade propeller (#1), (b) four-blade propeller (#2), (c) loop-type propeller (#3), (d) wide chord loop-type propeller (#4), and (e) DJI Phantom propeller (#5) at various rotational speeds.
Figure 10
Figure 10
Contour maps of the SPL in dB (Mic 2, θ=25 deg) over a frequency range of 6000–10,000 Hz associated with propeller noises: (a) two-blade propeller (#1), (b) four-blade propeller (#2), (c) loop-type propeller (#3), (d) wide chord loop-type propeller (#4), and (e) DJI Phantom propeller (#5) at various rotational speeds.
Figure 11
Figure 11
Comparison of the tonal noise, OASPLi (i=2, 4,, 36), below 5400 rpm at four locations of Mic 1 (a), Mic 2 (b), Mic 3 (c), and Mic 4 (d).
Figure 12
Figure 12
Comparison of the average broadband noise (OASPLband) beyond 6000 Hz vs. rotation speed at four locations of Mic 1 (a), Mic 2 (b), Mic 3 (c), and Mic 4 (d).
Figure 13
Figure 13
Comparison of noise loudness among the two-blade propeller (#1), four-blade propeller (#2), loop-type propeller (#3), wide chord loop-type propeller (#4), and DJI Phantom III propeller (#5) at a rotational speed of 5400 rpm (a) and at a stable thrust of 3 N (b).
Figure 14
Figure 14
Comparison of noise sharpness among the two-blade propeller (#1), four-blade propeller (#2), loop-type propeller (#3), wide chord loop-type propeller (#4), and DJI Phantom III propeller (#5) at a rotational speed of 5400 rpm (a) and at a stable thrust of 3 N (b).
Figure 15
Figure 15
Comparison of noise roughness among the two-blade propeller (#1), four-blade propeller (#2), loop-type propeller (#3), wide chord loop-type propeller (#4), and DJI Phantom III propeller (#5) at a rotational speed of 5400 rpm (a) and at a stable thrust of 3 N (b).
Figure 16
Figure 16
Comparison of fluctuation strength among the two-blade propeller (#1), four-blade propeller (#2), loop-type propeller (#3), wide chord loop-type propeller (#4), and DJI Phantom III propeller (#5) at a rotational speed of 5400 rpm (a) and at a stable thrust of 3 N (b).
Figure 17
Figure 17
Comparison of tonality among the two-blade propeller (#1), four-blade propeller (#2), loop-type propeller (#3), wide chord loop-type propeller (#4), and DJI Phantom III propeller (#5) at a rotational speed of 5400 rpm (a) and at a stable thrust of 3 N (b).
Figure 18
Figure 18
Comparison of psychoacoustic annoyance (Di’s model) among the two-blade propeller (#1), four-blade propeller (#2), loop-type propeller (#3), wide chord loop-type propeller (#4), and DJI Phantom III propeller (#5) at a rotational speed of 5400 rpm (a) and at a stable thrust of 3 N (b).
Figure 19
Figure 19
Mean psychoacoustic annoyance (Di’s model) vs. thrust and FM among the two-blade propeller (#1), four-blade propeller (#2), loop-type propeller (#3), wide chord loop-type propeller (#4), and DJI Phantom III propeller (#5) at a rotational speed of 3000–5700 rpm.

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