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author | krakenrf <78108016+krakenrf@users.noreply.github.com> | 2022-10-15 10:39:31 +0200 |
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committer | krakenrf <78108016+krakenrf@users.noreply.github.com> | 2022-10-15 10:39:31 +0200 |
commit | a2c3f2ab49f7b1c984692123390c61a002149179 (patch) | |
tree | ab674c12bf4da3e6e3ad1ff8edeca0bc92736bf6 | |
parent | Updated 08. Passive Radar (markdown) (diff) | |
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-rw-r--r-- | 08.-Passive-Radar.md | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/08.-Passive-Radar.md b/08.-Passive-Radar.md index f90279b..0a1d47b 100644 --- a/08.-Passive-Radar.md +++ b/08.-Passive-Radar.md @@ -102,7 +102,7 @@ Example cell 500, sampling rate 2.4 MHz and $N = 2^{22}$ $\mathrm{Bistatic Frequency (Hz)} = f_b = 500 * \frac{2400000}{2 \times 2^{22}} = 143 \mathrm{Hz}$ -Then to get to speed in m/s we simply multiple the Bistatic Frequency f_b with the wavelength of the illuminator, and multiply by -1. (Positive Doppler decreases the range between you and the target so it has negative speed, it is approaching) +Then to get to speed in $m.s^{-1}$ we simply multiple the Bistatic Frequency $f_b$ with the wavelength of the illuminator, and multiply by -1. (Positive Doppler decreases the range between you and the target so it has negative speed, it is approaching) So if we were using 560 MHz as our illuminator: |