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Journal of Sensor and Actuator Networks
  • Correction
  • Open Access

15 August 2025

Correction: Japertas et al. Experimental Study of Lidar System for a Static Object in Adverse Weather Conditions. J. Sens. Actuator Netw. 2025, 14, 56

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and
1
Transport Engineering Department, Kaunas University of Technology, K. Donelaičio St. 73, LT-44249 Kaunas, Lithuania
2
Faculty of Industrial Engineering and Technology, Lietuvos Inžinerijos Kolegija/Higher Education Institution, Tvirtovės al. 35, LT-50155 Kaunas, Lithuania
3
Faculty Electrical Engineering, Schmalkalden University of Applied Sciences, Blechhammer 4-9, D-98574 Schmalkalden, Germany
*
Authors to whom correspondence should be addressed.
There was an error in the original publication []. The number of the RMS value and the numbers of the Tables were inaccurate in Section 3.2, Paragraph 4, of the manuscript; the corrected text appears below.
From
However, using a 2 Hz LiDAR scan rate, the RMS at 1 m is 5 times smaller than the one under good weather conditions. This could be explained by the self-compensation effect on multiple paths due to heavy rain.
To
However, using a 2 Hz LiDAR scan rate, the RMS at 1 m is about 3 times smaller than the one under good weather conditions (Tables 1 and 3). This could be explained by the self-compensation effect on multiple paths due to heavy rain.
The numbers of RMS value were inaccurate, a correction has been made to Section 3.2, Paragraph 13:
From
For example, RMS at 1 m and 5.5 Hz is 4.42 mm, RMS at 1 m and 7 Hz is 8.18 mm, RMS at 6 m and 5.5 Hz is 27.35 mm and RMS at 6 m and 7 Hz is 23.93 mm. Thus, in rainy weather conditions, when the measured object is 6 m away, the scanning frequency of 5.5 Hz ensures about 5–6 times bigger errors (RMS) compared to the case when 2 Hz is used.
To
For example, RMS at 1 m and 5.5 Hz is 4.42 mm, RMS at 1 m and 7 Hz is 8.18 mm, RMS at 6 m and 5.5 Hz is 27.18 mm and RMS at 6 m and 7 Hz is 11.23 mm. Thus, in rainy weather conditions, when the measured object is 6 m away, the scanning frequency of 5.5 Hz ensures about 5–6 times smaller errors (RMS) compared to the case when 2 Hz is used.
The number of the RMS value was inaccurate; a correction has been made to Section 5, Paragraph 2:
From
When measuring the same object at a distance of 6–7 m, the errors also increase for the higher scan frequencies, but they are still 6 times smaller compared to the 2 Hz frequency already mentioned.
To
When measuring the same object at a distance of 6–7 m, the errors also increase for the higher scan frequencies, but they are still 4 times smaller compared to the 2 Hz frequency already mentioned.
The authors state that the scientific conclusions are unaffected. This correction was approved by the Academic Editor. The original publication has also been updated.

Reference

  1. Japertas, S.; Jankūnienė, R.; Knechtel, R. Experimental Study of Lidar System for a Static Object in Adverse Weather Conditions. J. Sens. Actuator Netw. 2025, 14, 56. [Google Scholar] [CrossRef]
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