To study the regular fluctuations of the geomagnetic field, monthly periodograms were constructed based on minute data from the Alma-Ata magnetic Observatory for the period from 2010 to 2018 by adding up the spectra of magnetically quiet days with a maximum daily Ap index of less than 5. Examples of periodograms for the X, Y and Z components of variations in the Earth's magnetic field are shown in Fig. 1 and Fig. 2. On the horizontal axis, the time UT in hours is shown (for Almaty, the local time UT + 6), on the vertical axis – the period of disturbances in minutes.
The constructed periodograms show that during the winter (January) and equinoctial (March, September) months at night, regular disturbances with periods from 70 to 110 minutes, the duration of which is about 2 hours, are present in the data on the X- and Y-components of the magnetic field. In July, during the daytime, regular disturbances with periods from 80 to 130 minutes are present in the data on the X-component of the magnetic field; there are no regular disturbances in the data on the Y-component. In the data on the Z-component of the magnetic field, regardless of the season, during the local pre-noon time of day (10–12 LT), there are regular disturbances with periods from 110 to 180 minutes, the duration of which is about 2–3 hours. The revealed periods are characteristic of acoustic-gravity waves generated in the auroral zones of the Northern and Southern hemispheres, regardless of the level of magnetic activity, and propagating from high latitudes to medium and low latitudes (Hocke and Schlegel, 1996; Vadas and Liu, 2009). The passage of the solar terminator is also a regular source of acoustic-gravity waves in the atmosphere (Somsikov et al., 2011).
3.2 Spectral analysis of the ULF geomagnetic data
To study ultra-low frequency fluctuations (ULF) of the geomagnetic field, 24 sets of 1-hour time series were formed for each day, each includes N = 3600 second values of the X-, Y-, Z-components of the geomagnetic field, and for them, we used the traditional method of Fast Fourier Transform FFT (Fast Fourier Transform, FFT) to calculate the values of the slope β of the spectrum. Technique to calculate the power spectral density of the ULF signals S(f ) given in the work of (Smirnova et al. 2001).
Examples of data processing by the FFT method for a local noon (12:00–13:00 LT) on a magnetically disturbed day on September 8, 2017, Kp = 8 are shown in Fig. 2 and when the geomagnetic conditions become quiet on October 4, 2017, Kp = 2, are shown in Fig. 3.
The variations of the X-, Y-, Z-components of the geomagnetic field with removed trend are shown, the straight line represents the slope of the β spectrum. The magnetically disturbed day (Kp = 8) was selected from the period of a very large magnetic storm that occurred on September 6–9, 2017. According to NASA's Solar Dynamics Observational Laboratory (https://sdo.gsfc.nasa.gov/) the magnetic storm was caused by a series of solar flares, including the X9.3 flare, the most intense flare recorded during the current solar cycle.
On a perturbed day (the geomagnetic storm) in local time interval of 12–13 hours, the amplitude of the perturbations is largest for X-component, it reach 5–15 nT with periods from 2 to 5 min. The slope of the spectrum, β is 3.84, 3.95 and 3.13, calculated from the X-, Y-, Z-components, respectively. On a geomagnetic quiet day, in local time interval of 12–13 hours, the amplitude of disturbances is largest in Z-component, it reach 0.5 nT with periods of less than 1 min. The slope of the β spectrum is 2.55, 2.99 and 2.08, calculated from the X-, Y-, Z-components, respectively, which corresponds to the fractional Brownian motion in geomagnetic quiet day (Smirnova et al. 2001).
ULF disturbances with amplitudes from tenths to tens of Nt and are divided into regular geomagnetic pulsations, Pc, and irregular, pulsed, Pi. Depending on the periods, geomagnetic pulsations are classified as follows: Pc1 (T = 0.2-5 c), Pi1 (T = 1–40 c); Pc2 (T = 5–10 c), Pi2 (T = 40–150 c); Pc3 (T = 10–45 c), Pi3 (T > 150 c); Pc4 (T = 45–150 c); Pc5 (T = 150–600 c); Pc6 (T > 600 c).
The question on the nature of generating regular pulsations of the geomagnetic field remains open today. Waves in the transition region between the solar wind and the magnetosphere can serve as a powerful source of magnetic pulsations (Schott et al. 2004). The resonant excitation of Pc3-Pc5 pulsations in the Earth's magnetosphere has been repeatedly discussed in the literature. Some authors explain the often observed harmonic structure of Pc3-Pc4 spectra after sudden onset magnetic storms (SC) by resonance effects (Kleimenova and Kozyreva, 2014). A number of papers discuss the possibility of direct transfer of Pc5 pulsations from the solar wind to the magnetosphere, while the spectrum of pulsations may differ from the resonant frequencies of the magnetosphere (Villante et al. 2003; Kessel et al. 2004). Pi pulsations are typical for night hours and for periods of geomagnetic disturbances.