Bistatic Cross Section
Understanding Bistatic RCS
In conventional (monostatic) radar, the transmitter and receiver share the same antenna. The target's radar cross section describes how much energy is scattered directly back toward the radar. Bistatic configurations separate the transmitter and receiver, viewing the target from two different angles. This reveals scattering information invisible to monostatic radar and creates unique tactical advantages.
The most dramatic effect occurs near forward scatter (β approaching 180°), where every target, regardless of stealth shaping, produces a large scatter lobe proportional to its physical silhouette area. This fundamental physics principle means that stealth aircraft optimized to minimize backscatter remain detectable by properly positioned bistatic receivers.
Bistatic RCS Equations
σB = lim(R→∞) 4πR² · |Es|²/|Ei|²
Forward Scatter RCS:
σfwd = 4πA²/λ²
A = projected cross-sectional area
Kell's Equivalence Theorem:
σB(θi,θs) ≈ σM(θbisector)
at feq = f · cos(β/2)
Bistatic Doppler:
fD = (v/λ)[cos(δT) + cos(δR)]
Scattering Region Characteristics
| Region | β Range | RCS vs. Monostatic | Dominant Mechanism |
|---|---|---|---|
| Backscatter | < 5° | ≈ σM | Specular, edges, creeping waves |
| Bistatic | 5–150° | Variable | Specular, diffraction |
| Forward scatter | > 150° | ≫ σM | Babinet shadow (A²/λ²) |
Bistatic Radar Applications
| Application | Illuminator | Advantage | Limitation |
|---|---|---|---|
| Passive radar (PCL) | FM/DVB-T/cellular | Covert, low cost | Resolution, geometry |
| Forward-scatter fence | Dedicated TX | Anti-stealth | Baseline proximity |
| Multistatic network | Shared TX | Glint averaging, ECM-hard | Synchronization |
| Bistatic SAR | Satellite | No TX on RX platform | Geometry constraints |
Frequently Asked Questions
vs. monostatic RCS?
Monostatic = backscatter only (β=0). Bistatic reveals angle-dependent scattering. Forward scatter (β→180°): σfwd = 4πA²/λ², can be 60+ dB above stealth monostatic RCS. Kell's theorem relates them for smooth targets at small β.
Kell's theorem?
σB(β) ≈ σM(β/2) at feq = f·cos(β/2). Valid for smooth, electrically large targets with β < 40–60°. Fails for edges, cavities, resonance, and forward scatter. Enables bistatic estimation from monostatic databases.
Bistatic radar applications?
Passive radar (PCL): covert detection using FM/DVB-T illuminators. Forward-scatter fencing: anti-stealth detection via physical silhouette. Multistatic: improved detection + ECM resistance from spatial diversity. Bistatic SAR: satellite TX with ground/airborne RX.