3.2. Seismic Noise and Its Variation
Seismic noise was analyzed for all six stations installed in the near zone. The calculation method used is described in [
7]. The analysis was done by steps:
- selection of recording segments for the same periods of time for day (6-7 a.m. GMT) and night (4-5 p.m. GMT). The segments were 10 minutes long, and records without events were selected, with 10 segments separately for day and night;
- calculation of the spectral characteristics of noise for each station, for each component, separately for daytime and night-time periods;
- calculation of average (median) spectral curves (noise models) for each station, each component, for day and night; - comparison of results with Peterson’s global noise models [
8] and between data from all stations in the near zone.
Below are summary graphs of the spectral power density of seismic noise for all stations for night time (
Figure 10). The black lines show the standard high-level and low-level seismic noise curves (High Noise Model and Low Noise Model) according to Peterson [
7] that allow the noise level to be assessed relative to global models.
A comparison of daytime and night-time noise level shows a clear pattern in noise variations throughout the day. The daytime noise level is higher than the night-time level at frequencies above 5 Hz at all stations except the Merzbacher station. The Merzbacher station also has the lowest noise level (
Figure 11). However, a slight increase in daytime noise is noticeable at this station at frequencies close to 1 Hz. A low noise level is also observed at the Podgornoye station. The equipment at these two permanent stations is installed in bunkers on a rock foundation. However, the equipment at the field stations is installed in seismic vaults of 40-50 cm depth.
Figure 12 shows seismograms from field stations for one day, Z components. The station traces in the Figure are arranged from top to bottom according to their distance from the glacial zone (60 km Bayankol, 75 km Shynybek, 135 km Karkara).
The analysis of diurnal seismic records from three field stations clearly shows, even without any processing, a difference in seismic noise levels between day and night hours. Approximately at 13-14 hours GMT (18-19 hours local time), the noise level changes significantly: it becomes lower (the width of the dark part of the vibration trace narrows). This effect is more pronounced at the Shynybek and Karkara stations and less at the Bayankol station. The vertical lines on all traces are glacial seismic events, the exact number of which cannot be calculated. The number of seismic events decreases with distance from the glaciers.
Figure 12 shows the similar diurnal seismic oscillations from Merzbacher station. The almost complete absence of visible daily variations in seismic noise is noteworthy. The width of the “dark” band remains almost unchanged throughout the day.
The possible reason is significantly different locations of the stations and different conditions of the equipment installation. Seismic noise level at field stations is affected by increased general noise from transport, operation of various devices, and agricultural activity in villages during daylight hours, which is completely absent at the altitude of the Merzbacher station (3304 m). In addition, at the Merzbacher station, the equipment is installed in a 2 m bunker, while at other stations, the equipment is installed in seismic vaults of 40-50 cm depth. This excludes the influence of wind interference on the seismic noise level.
The data analysis also showed the noticeable increase in glacial events number after 15:00 GMT (evening and night local time). This phenomenon is also confirmed by the results of all network data processing: the diurnal number of glacial earthquakes clearly depends on temperature change.
In cases when actual physical characteristics of the oscillations are known from seismic noise recordings, the minimum expected magnitudes and energy classes of glacial earthquakes can be estimated upon detection. The following well-founded assumptions were used. It was assumed that the amplitude of the signal in P-waves should exceed the amplitude of seismic noise by three times, and the amplitude of S-waves should be approximately twice the amplitude of P-waves.
Figure 13 shows the waveforms for all stations in the near zone. However, all stations of the IGR NNC RK network record velocity, while the Merzbacher CAIES station records ground displacement.
Formulas for estimating the regional magnitude mpv [
9] and energy class K [
10] for Tien Shan earthquakes were used for the calculations. Since significant variations in oscillations during the day have been established, the calculations were performed for day and night. The night records show the smaller earthquakes clearer than the day time records due to the noise variations.
The energy class is calculated using the formula K = 1.8⋅log10 (Ap+As) + Ω(Δ,km), where Ap and As are the maximum amplitudes of longitudinal and transverse seismic waves measured in microns on the SKM channel, Ω is a calibration function describing the attenuation of seismic waves, depending on the epicentral distance. Magnitude mpv = log10(Ap/T)+σ(Δ,km). Ap and T are the amplitude and corresponding period in the displacements of the longitudinal wave of ground vibrations, σ(Δ,km) is the calibration function for Ap/T describing the attenuation of the vibration velocity depending on the epicentral distances. Note that for the Merzbacher station, it is not necessary to convert from velocities to ground displacements when calculating using these formulas, since we had displacement records as input.
The obtained results of predicted sensitivity of the established monitoring network are shown in
Table 3 and
Table 4.
The analysis of seismic noise records from all stations installed in the near zone allow assuming that the network is capable to detect and locate glacial events of mpv ~2-2.5 and energy class of 5-6.
3.3. Analysis of Meteorological, Infrasound, and Seismic Data
For meteorological observations at the Bayankol (BNK), Karkara (KRK) and Shynybek (SHN) stations, a compact “Gill Maximet GMX 500” weather station able to record five basic parameters was used:
1. Wind speed (LWS), measurement unit – m/s.
2. Wind direction (LWD), measurement unit – ⁰ northward.
3. Temperature (LKO), measurement unit – ⁰С.
4. Relative humidity (LIO), measurement unit – %.
5. Atmospheric pressure (LDO), measurement unit – mm Hg.
Based on meteorological data, wind roses, daily and seasonal changes in wind speed were studied for each station. The results of the meteorological data analysis are shown by the example of the Bayankol (BNK) station. Examination of the combined graphs of wind direction and speed allowed determining regular periodic changes in wind direction, characterized by relative stability in the evening and night-time periods. In most cases, changes in wind direction coincide with an increase in wind speed. The prevailing wind speed ranges from 0.3 to 1.5 m/s, with an increase to 9.6 m/s during changes in direction. This analysis was performed every ten days during the entire observation period.
Then, the wind rose diagrams were constructed and analyzed for the Bayankol (BNK) station. The diagrams are divided into 16 sectors, each covering a direction equal to 22.5°. The prevailing wind direction, for example, in December 2024, is 180–202.5°, followed in intensity by 202.5–225° and 157.5–180°. There is almost no wind from the direction 315–45° to the area of glacial seismicity.
Figure 14 schematically shows the wind direction relative to the station location. Long bold arrows indicate the direction during the night breeze, long thin arrows indicate the wind direction during the daytime breeze, and short thin arrows indicate a light wind during the change of main directions. The background of the figure is a satellite image.
The Figure shows that the prevailing wind direction coincides with the direction of the Akkol Gorge, where the station is located. The azimuth of the Akkol Gorge is 195°, which is consistent with the wind rose diagram. The azimuth of the Bayankol Gorge that adjoins the Akkol Gorge, is 120° at the point of junction, with a further change in azimuth to 355° in a northerly direction and subsequent exit into the foothill valley (not all of the area is shown in the figure).
Basing on the results of the wind regime analysis at the station’s site over the year, the following can be stated:
- In general, the wind regime is relatively stable and predictable, except for periods when there are sudden changes in weather conditions (cyclones, anticyclones, etc.);
- The main direction of air mass movement in the surface layer during night and day breezes coincides with the direction of the gorge.
- Wind speed is mainly within the range of 2–4 meters per second, increasing to 8–10 meters per second during the transition from night breeze to day breeze, with gusts of up to 16 meters per second.
- The daily cycle is roughly as follows: from 4 p.m. to 7:30 a.m. local time the next day (evening, night and early morning), air masses move down along the Akkol Gorge, exiting into the Bayankol Gorge and further into the foothill valley. These are descending flows of air cooled overnight. Then, from 7:30 to 10:00, there is a temporary сфдь, during which the wind direction changes. From 10:00 to 14:00, the air warmed in the valley begins to rise into the mountains, the wind speed increases, and the direction changes to almost the opposite. From 14:00 to 16:00, calm returns, the wind changes speed and direction, and the cycle repeats;
- During sudden weather change (cyclone, anticyclone), the direction and speed of the wind change chaotically;
- There is practically no wind from the north-west and north directions, as there is a dead-end gorge in this direction that only leads to the Akkol Gorge.
A comparison of wind diagrams from all field stations shows that the main direction of surface winds at the Karkara and Bayankol stations is almost perpendicular to the direction of the research object, which makes it unlikely that infrasound signals generated by the glaciers of the central Tien Shan Mountains will be detected. The main wind direction at the Shynybek station not only corresponds well with the direction of the glaciers, but also covers almost the entire area of the high-mountainous Tien Shan. Thus, most probably, the Shynybek station will detect infrasound signals from glacial phenomena not only reflected from the stratosphere, but also directly from glaciers, compared to the Karkara and Bayankol stations.
The analysis of infrasound stations records revealed very intense fluctuations throughout each day. Detailed examination of combined infrasound and meteorological data revealed patterns in the periodicity of acoustic noise.
Figure 15 shows a three-day record of microbarometer signals (Bayankol station). The recording began at 00:00 on 30 May 2024 and ended at 23:59 on 1 June 2024 (GMT). The upper trace is the microbarometer record, and the lower trace is the recording from the temperature sensor installed at the same site.
Figure 15 shows that the onset of intense acoustic noise clearly correlates with the air temperature increase at the microbarometer installation site. The time from the temperature rise beginning to the appearance of intense acoustic noise is about two and a half to three hours. The duration of intense acoustic noise is, on average, about nine and a half to eleven hours per day. The average background noise level at night is about 18 mV, and during the day it is 570 mV.
This pattern is observed daily throughout the entire observation period complicating significantly the detection of infrasound events during the daytime against the background of interference. The time of the temperature increase beginning, the strengthening in wind speed, and the time of strong infrasound interference and its duration on the microbarometer records are completely synchronized. Thus, it can be concluded that the increase of the acoustic interference intensity on the microbarometer records is a consequence of meteorological parameters change at the equipment installation site.
Figure 16 and
Figure 17, represented below, show that the time of wind speed increase and the time of start and duration of intensive infrasound noise are completely synchronous on the microbarometer records.
Figure 18 shows a summary graph of temporal changes by a set of data from a multi-parameter system. Three components of seismic station records, temperature records, and infrasound station records are shown.
There is a correlation between the occurrence of infrasound and seismic noise and daily temperature changes. For infrasound vibrations, this correlation occurs due to the changes in wind parameters as a result of daily temperature increase; for seismic vibrations, the temperature increase after sunrise determines the overall level of cultural interference increase due to human activity at the station’s location area, increased traffic on the roads, the start of agricultural work in the fields, etc. The wind impact on the field stations equipment installed in seismic vaults also cannot be denied.
Basing on the conducted analysis, an important methodological conclusion was made regarding the detectability of infrasound signals from glaciers: the most promising station for its detection is Shynybek that is characterized by the wind direction directly from the zone of glacial earthquakes. The infrasound signals are better to be searched outside the period of intense daytime noise associated with temperature and wind changes. This period can be predicted quite accurately.
As the number of the infrasound stations used (1 and later 2) did not allow analyzing its data as array and apply, for example, the PMCC technique [
11], the azimuth of signal arrival and apparent velocity, all further processing of infrasound data was based on the association of infrasound signals with data from the seismic bulletin of glacial earthquakes. For further monitoring of glaciers, it is recommended to install an infrasound array consisting of at least three microbarometers and apply infrasound wave path modelling to select the best site for infrasound recording.
During the glacial seismicity monitoring network operation, more than 4,000 seismic events have been recorded and processed at the Data Centre. A seismic bulletin has been compiled. A map of the located events epicenters is shown in
Figure 19. Within the area of the large-scale glaciers of the High Tien Shan that has linear dimensions of more than 200 km, a zone of high seismic activity with clear boundaries and structure is clearly distinguished. The events with the minimum magnitude mpv were recorded by the Bayankol station – mpv=0.9. Events with mpv=2.0 were detected and located without omission. The analysis of the identified patterns of glacial seismic events is beyond the scope of this paper.