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Radar Range Equation Calculator

Calculate maximum radar detection range from peak power, antenna gain, RCS, noise figure, and bandwidth using the radar equation. Free, instant results.

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Formula

Rmax=(PtG2λ2σ/((4π)3Pmin))(1/4)R_max = (Pt·G²·λ²·σ / ((4π)³·Pmin))^(1/4)
R_maxMaximum detection range (m)
PtPeak transmit power (W)
GAntenna gain (linear)
λWavelength (m)
σRadar cross section (m²)
PminMinimum detectable signal (kTBF) (W)

How It Works

The Radar Range Equation calculates maximum detection distance for a given target — the foundation of every radar system design from airport surveillance to automotive collision avoidance. Defense contractors, aviation authorities, and automotive engineers use this to specify transmitter power, antenna size, and receiver sensitivity.

The standard form from Skolnik's Radar Handbook (IEEE Press): R_max = [(P_t·G²·λ²·σ) / ((4π)³·S_min)]^(1/4), where P_t is peak power, G is antenna gain, λ is wavelength, σ is radar cross-section (RCS), and S_min is minimum detectable signal. The fourth-root relationship means doubling range requires 16× the power — a critical constraint in radar design.

Typical RCS values (Skolnik, IEEE): commercial aircraft 10–100 m², fighter jet 1–10 m², cruise missile 0.1–1 m², stealth aircraft 0.001–0.01 m², bird 0.001–0.01 m². Weather radar detects precipitation with RCS of 10⁻¹⁴ m² per cubic meter of rain. For automotive radar (77 GHz), pedestrian RCS is 0.5–2 m², bicycle 1–3 m², car 10–100 m². Detection probability of 90% (P_d = 0.9) with false alarm rate of 10⁻⁶ requires SNR of 13.2 dB per Swerling I target model.

Worked Example

Airport surveillance radar (ASR-11 class) detecting Boeing 737 at 100 nmi

Given (typical S-band ASR specs):

  • Peak power P_t = 25 kW (44 dBW)
  • Antenna gain G = 34 dBi (4.3 m aperture)
  • Frequency f = 2.8 GHz → λ = 0.107 m
  • Target RCS σ = 30 m² (Boeing 737, head-on)
  • Required SNR = 13.2 dB for P_d = 0.9, P_fa = 10⁻⁶
  • System noise figure NF = 3 dB, Bandwidth B = 1 MHz
Step 1: Noise floor N = kTB·NF = −174 + 60 + 3 = −111 dBm

Step 2: S_min = N + SNR = −111 + 13.2 = −97.8 dBm (16.6 fW)

Step 3: R = [(25000 × 2512² × 0.107² × 30) / ((4π)³ × 1.66×10⁻¹⁴)]^0.25 = 185 km (100 nmi)

Verifies ASR-11 spec: 60 nmi primary, 120 nmi secondary with transponder.

Practical Tips

  • Apply 4th-root rule: 16× power for 2× range, 256× power for 4× range — explains why long-range radar uses megawatt transmitters
  • Add 6–10 dB atmospheric loss for X-band (10 GHz) beyond 100 km; use ITU-R P.676 for precise attenuation vs. frequency
  • Account for pulse integration: N coherent pulses improve SNR by 10·log₁₀(N) dB. 100 pulses = 20 dB improvement
  • Clutter-limited radars: noise floor replaced by clutter return, typically −40 to −60 dBsm/m² for land, −50 to −70 dBsm/m² for sea (Skolnik)

Common Mistakes

  • Using peak power instead of average power for duty-cycle-limited systems — a 1% duty cycle reduces effective power by 20 dB
  • Ignoring antenna pattern losses: typical −3 dB beamwidth captures only 50% of target time, adding 3 dB effective loss
  • Assuming constant RCS: real targets fluctuate ±10 dB (Swerling models). Use statistical P_d curves, not deterministic SNR
  • Forgetting two-way propagation: radar suffers R⁴ loss (not R²) because signal travels to target AND back

Frequently Asked Questions

Transmitted power and antenna gain dominate (both to 1/4 power in range). Doubling antenna aperture increases range by 41% (2^0.5). Reducing noise figure from 6 dB to 3 dB improves range by 19%. RCS is target-dependent and often the limiting uncertainty — a 10 dB RCS reduction (stealth) cuts detection range by 44%.
RCS scales roughly with physical cross-section but depends heavily on shape and materials. A flat plate reflects 30+ dB more than a sphere of equal area at normal incidence. Stealth aircraft use faceting and RAM (radar-absorbing material) to reduce RCS from 10 m² to 0.001 m² — requiring 100× closer approach for detection.
Monostatic (co-located TX/RX) uses R⁴ in denominator. Bistatic (separated TX/RX) uses R_tx²·R_rx², which can improve range when target is between stations. Bistatic RCS differs from monostatic — forward scatter RCS can exceed backscatter by 10–20 dB for conducting objects at certain geometries.
Rain attenuation per ITU-R P.838: at 10 GHz, 10 mm/hr rain causes 0.1 dB/km one-way (0.2 dB/km two-way). At 77 GHz automotive radar, heavy rain (25 mm/hr) causes 10 dB/km — limiting effective range to ~100 m. Always add two-way path loss for weather effects.

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