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NV5 Geospatial Blog

Each month, NV5 Geospatial posts new blog content across a variety of categories. Browse our latest posts below to learn about important geospatial information or use the search bar to find a specific topic or author. Stay informed of the latest blog posts, events, and technologies by joining our email list!



Easily Share Workflows With the Analytics Repository

Easily Share Workflows With the Analytics Repository

10/27/2025

With the recent release of ENVI® 6.2 and the Analytics Repository, it’s now easier than ever to create and share image processing workflows across your organization. With that in mind, we wrote this blog to: Introduce the Analytics Repository Describe how you can use ENVI’s interactive workflows to... Read More >

Deploy, Share, Repeat: AI Meets the Analytics Repository

Deploy, Share, Repeat: AI Meets the Analytics Repository

10/13/2025

The upcoming release of ENVI® Deep Learning 4.0 makes it easier than ever to import, deploy, and share AI models, including industry-standard ONNX models, using the integrated Analytics Repository. Whether you're building deep learning models in PyTorch, TensorFlow, or using ENVI’s native model creation tools, ENVI... Read More >

Blazing a trail: SaraniaSat-led Team Shapes the Future of Space-Based Analytics

Blazing a trail: SaraniaSat-led Team Shapes the Future of Space-Based Analytics

10/13/2025

On July 24, 2025, a unique international partnership of SaraniaSat, NV5 Geospatial Software, BruhnBruhn Innovation (BBI), Netnod, and Hewlett Packard Enterprise (HPE) achieved something unprecedented: a true demonstration of cloud-native computing onboard the International Space Station (ISS) (Fig. 1). Figure 1. Hewlett... Read More >

NV5 at ESA’s Living Planet Symposium 2025

NV5 at ESA’s Living Planet Symposium 2025

9/16/2025

We recently presented three cutting-edge research posters at the ESA Living Planet Symposium 2025 in Vienna, showcasing how NV5 technology and the ENVI® Ecosystem support innovation across ocean monitoring, mineral exploration, and disaster management. Explore each topic below and access the full posters to learn... Read More >

Monitor, Measure & Mitigate: Integrated Solutions for Geohazard Risk

Monitor, Measure & Mitigate: Integrated Solutions for Geohazard Risk

9/8/2025

Geohazards such as slope instability, erosion, settlement, or seepage pose ongoing risks to critical infrastructure. Roads, railways, pipelines, and utility corridors are especially vulnerable to these natural and human-influenced processes, which can evolve silently until sudden failure occurs. Traditional ground surveys provide only periodic... Read More >

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Calculating the period of the sunspot cycle

Anonym

Two weeks ago, I used the sunspot number data provided by the Solar Physics Group at NASA's Marshall Space Flight Center to demonstrate positioning plots in window. This week, I'd like to show how to calculate the period of the sunspot cycle. If you haven't already done so, download the sunspot numbers file and place it in your IDL path. Read it with the astrolib READCOL procedure:

 file = file_which('spot_num.txt', /include) readcol, file, year, month, sunspots

Next, transform the sunspot series to the frequency domain and compute magnitude and power spectra:

 mspec = abs(fft(sunspots)) pspec = mspec^2

(Aside: FFT: it's all you need.) I'd like to display the power spectrum as a function of frequency. This requires a few statements to set up a frequency vector based on the time data from the sunspot numbers file:

 sampling_interval = 1/12.0 ; years, from file freq_nyquist = 0.5/sampling_interval ; years^{-1} n_sunspots = n_elements(sunspots) freq = findgen(n_sunspots/2)/(n_sunspots/2-1)*freq_nyquist

The sampling interval is one month. This allows me to determine the Nyquist frequency (the maximum resolvable frequency), which along with the number of sunspots in the file, gives me the information to define a frequency vector. Note that I'm defining only positive frequencies up to the Nyquist frequency; this is because I'm going to display a one-sided power spectrum. Fold the negative Fourier modes into the spectrum, omitting the zero (DC) mode:

 freq_nodc = freq[1:n_sunspots/2-1] pspec_nodc = 2*pspec[1:n_sunspots/2-1]

and display the result on logarithmic axes:

 p = plot(freq_nodc, pspec_nodc, /xlog, /ylog, $ xtickunits='exponent', $   ; IDL 8.2.1 xtitle='Frequency ($yr^{-1}$)', $ ytitle='Spectral Density', $ title='Power Spectrum of Sunspot Numbers, 1749-2010')

Note that I can set the style of tick units on the axes: 'exponent' and 'scientific' are new in IDL 8.2.1. The power spectrum has a peak near 0.1 yr^{-1}. Locate the peak frequency with MAX and mark it on the plot with POLYLINE:

 pspec_nodc_peak = max(pspec_nodc, i_peak) freq_nodc_peak = freq_nodc[i_peak] !null = polyline([1.0,1.0]*freq_nodc_peak, p.yrange, color='orange', /data)

The inverse of the peak frequency gives the period of the sunspot cycle: approximately 11 years. Mark this on the plot with TEXT:

 sunspot_peak_period = 1.0/freq_nodc_peak str = '$T_{peak}$ = ' + strtrim(sunspot_peak_period,2) + ' years' !null = text(1e-1, 1e-4, str, /data)

Here's my result:

Power spectrum of sunspot numbers time series. Data courtesy NASA.

Finally, just because it's interesting, test Parseval's theorem (energy is conserved in the time- and frequency-domain representations of the signal) in several forms:

 IDL> print, total(pspec)*n_sunspots, total(sunspots^2) 1.46437e+007 1.46437e+007 IDL> print, mspec[0], mean(sunspots) 52.0133      52.0134 IDL> print, total(pspec[1:*]), stddev(sunspots)^2*(n_sunspots-1)/n_sunspots ; convert from sample variance 1965.67      1965.66

Conservation of greatness (of FFT)!

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