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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!



Mapping Earthquake Deformation in Taiwan With ENVI

Mapping Earthquake Deformation in Taiwan With ENVI

12/15/2025

Unlocking Critical Insights With ENVI® Tools Taiwan sits at the junction of major tectonic plates and regularly experiences powerful earthquakes. Understanding how the ground moves during these events is essential for disaster preparedness, public safety, and building community resilience. But traditional approaches like field... Read More >

Comparing Amplitude and Coherence Time Series With ICEYE US GTR Data and ENVI SARscape

Comparing Amplitude and Coherence Time Series With ICEYE US GTR Data and ENVI SARscape

12/3/2025

Large commercial SAR satellite constellations have opened a new era for persistent Earth monitoring, giving analysts the ability to move beyond simple two-image comparisons into robust time series analysis. By acquiring SAR data with near-identical geometry every 24 hours, Ground Track Repeat (GTR) missions minimize geometric decorrelation,... Read More >

Empowering D&I Analysts to Maximize the Value of SAR

Empowering D&I Analysts to Maximize the Value of SAR

12/1/2025

Defense and intelligence (D&I) analysts rely on high-resolution imagery with frequent revisit times to effectively monitor operational areas. While optical imagery is valuable, it faces limitations from cloud cover, smoke, and in some cases, infrequent revisit times. These challenges can hinder timely and accurate data collection and... Read More >

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 >

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4.5

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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