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Free-space path loss
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== Free-space path loss in decibels == A convenient way to express FSPL is in terms of [[decibel]]s (dB):<ref name="Pasternack">{{cite web |title=Free Space Path Loss Calculator |url=https://www.pasternack.com/t-calculator-fspl.aspx |website=Pasternack |access-date=October 16, 2021}}</ref> :<math> \begin{align} \operatorname{FSPL}(\text{dB}) &= 10\log_{10}\left(\left(\frac{4\pi d f}{c}\right)^2\right) \\ &= 20\log_{10}\left(\frac{4\pi d f}{c}\right) \\ &= 20\log_{10}(d) + 20\log_{10}(f) + 20\log_{10}\left(\frac{4\pi}{c}\right) \\ &= 20\log_{10}(d) + 20\log_{10}(f) -147.55, \end{align} </math> using [[SI unit]]s of meters for <math>d</math>, [[hertz]] (s<sup>β1</sup>) for <math>f</math>, and meters per second (mβ s<sup>β1</sup>) for <math>c</math>, (where c=299 792 458 m/s in vacuum, β 300 000 km/s) For typical radio applications, it is common to find <math>d</math> measured in [[kilometers]] and <math>f</math> in [[gigahertz]], in which case the FSPL equation becomes :<math>\operatorname{FSPL}(\text{dB}) = 20\log_{10}(d_{km}) + 20\log_{10}(f_{GHz}) + 92.45,</math> an increase of 240 dB, because the units increase by factors of {{10^|3}} and {{10^|9}} respectively, so: :<math>20\log_{10}(10^{3}) + 20\log_{10}(10^{9}) = 240.</math> (The constants differ in the second decimal digit when the speed of light is approximated by 300 000 km/s. Whether one uses 92.4, 92.44 or 92.45 dB, the result will be OK as the average measurement instruments cannot provide more accurate results anyway. A logarithmic scale is introduced to see the important differences (i.e. order of magnitudes), so in engineering practice dB results are rounded)
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