Where the energy goes — rays off one shape, radar on the left
Returned to the radarSent elsewhereShape, with its normal or bisector
σ vs angle — physical optics at X-band (dBsm)
Sent back to the radar
—
—
Peak σ
—
—
—
With aspect
—
Verdict
—
—
Rays: geometric optics, where the energy goes (returned = within 2° of the radar's line of sight). Curve: physical optics, how much comes back, for a 0.5 m square plate, a dihedral of two 0.5 m square faces and a sphere of the same 0.25 m² projected area at X-band (λ = 3 cm); shadowing and edge diffraction ignored.
Notional faceted-target RCS vs aspect — 0° = nose-on, clockwise
RCS pattern (dBsm)Selected sector
Type-along: single-number candidates by sector (dBsm)
Sector
Samples
Max
Median
Mean (linear)
Max
—
brightest flash
Median
—
the floor you see
Mean (linear)
—
10·log₁₀(mean σ)
—
A search radar sweeping past sees the floor most of the time, so the median prices detection range (R ∝ σ1/4). The spikes are brief, real flashes — but hard to track on. Neither number is wrong; they answer different questions.
Detection footprints vs heading — top-down plan view (km)
Radar holds a trackSafe (outside its detection footprint)Aircraft heading
—
Per-radar exposure
Site
Aspect
σ (dBsm)
R_det (km)
Range (km)
RCS is a pattern, not a number — so orientation is survivability. Each radar sees a different aspect, and Block 1's monostatic law Rdet ∝ σ1/4 turns that aspect into a detection range. Point your low-RCS nose or tail at the threat that matters and its footprint pulls away; swing a spike onto it and a needle runs over you.