EW Academy · Contents · Chapter 5 · §5.6 · Nederlandse versie

§5.6 Inverse square law

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In plain terms

If you stand twice as far from a lamp, four times less light falls on you. A radar echo has to travel that path twice — out to the target and back — and so becomes weaker very rapidly with distance.

In practice

That is why the radar warning receiver (RWR) in a combat aircraft usually hears an enemy radar well before that radar can see the aircraft (Radar Warning Receiver (RWR)). The signal to the RWR only has to travel one way. The pilot therefore knows there is a radar before the radar knows there is an aircraft.

Energy leaving an antenna spreads out over an ever larger spherical surface. Because the area of a sphere grows with R², the power density decreases with the square of the distance — the inverse square law:

power density ∝ 1 / R² 2× as far away → 4× as weak; 10× as far → 100× as weak
Inverse square law: a source S radiates through surfaces at distance r, 2r and 3r; the same energy spreads over 1, 4 and 9 squares.
The inverse square law: at 2r and 3r the same amount of energy spreads over 4× and 9× as much area respectively. Image: Borb / Wikimedia Commons — CC BY-SA 3.0.

For radar it is worse. The signal has to travel out and back, and the target behaves like a new (weak) transmitter. On the way out 1/R² applies, on the way back another 1/R². The received echo power therefore decreases with the fourth power of the distance:

Preceived ∝ 1 / R⁴ the simplified radar equation: Pr = (Pt × G² × λ² × σ) / ((4π)³ × R⁴) Pt = transmit power, G = antenna gain, λ = wavelength, σ = RCS, R = distance

The consequences are far-reaching:

Example

A radar detects a target with an RCS of 10 m² at 200 km. The same target with stealth measures (RCS 0.001 m², a factor of 10,000 smaller) is only seen at 200 / ⁴√10,000 = 200 / 10 = 20 km.