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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!



Not All Supernovae Are Created Equal: Rethinking the Universe’s Measuring Tools

Not All Supernovae Are Created Equal: Rethinking the Universe’s Measuring Tools

6/3/2025

Rethinking the Reliability of Type 1a Supernovae   How do astronomers measure the universe? It all starts with distance. From gauging the size of a galaxy to calculating how fast the universe is expanding, measuring cosmic distances is essential to understanding everything in the sky. For nearby stars, astronomers use... Read More >

Using LLMs To Research Remote Sensing Software: Helpful, but Incomplete

Using LLMs To Research Remote Sensing Software: Helpful, but Incomplete

5/26/2025

Whether you’re new to remote sensing or a seasoned expert, there is no doubt that large language models (LLMs) like OpenAI’s ChatGPT or Google’s Gemini can be incredibly useful in many aspects of research. From exploring the electromagnetic spectrum to creating object detection models using the latest deep learning... Read More >

From Image to Insight: How GEOINT Automation Is Changing the Speed of Decision-Making

From Image to Insight: How GEOINT Automation Is Changing the Speed of Decision-Making

4/28/2025

When every second counts, the ability to process geospatial data rapidly and accurately isn’t just helpful, it’s critical. Geospatial Intelligence (GEOINT) has always played a pivotal role in defense, security, and disaster response. But in high-tempo operations, traditional workflows are no longer fast enough. Analysts are... Read More >

Thermal Infrared Echoes: Illuminating the Last Gasp of a Dying Star

Thermal Infrared Echoes: Illuminating the Last Gasp of a Dying Star

4/24/2025

This blog was written by Eli Dwek, Emeritus, NASA Goddard Space Flight Center, Greenbelt, MD and Research Fellow, Center for Astrophysics, Harvard & Smithsonian, Cambridge, MA. It is the fifth blog in a series showcasing our IDL® Fellows program which supports passionate retired IDL users who may need support to continue their work... Read More >

A New Era of Hyperspectral Imaging with ENVI® and Wyvern’s Open Data Program

A New Era of Hyperspectral Imaging with ENVI® and Wyvern’s Open Data Program

2/25/2025

This blog was written in collaboration with Adam O’Connor from Wyvern.   As hyperspectral imaging (HSI) continues to grow in importance, access to high-quality satellite data is key to unlocking new insights in environmental monitoring, agriculture, forestry, mining, security, energy infrastructure management, and more.... 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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