Dead Zone
Where the Blind Range Comes From
Any sensor that shares one aperture between transmit and receive must protect its receiver while the high-power pulse is on the line. In a pulsed radar a transmit/receive switch and a T/R limiter blank the receiver for the duration of the pulse plus a short recovery interval. An echo that returns during this window is partly or wholly lost, an effect called eclipsing. The result is a near-range hole: the radar simply cannot report a target closer than the range corresponding to the round-trip time of one pulse width. This minimum range is the most common meaning of dead zone in microwave engineering, and it is set entirely by the uncompressed pulse width rather than by signal-to-noise ratio.
Pulse compression complicates the picture. A long transmit pulse carries the energy needed for detection range, but the dead zone is governed by the physical length of that transmit pulse, not by the compressed range resolution. A radar that transmits a 10 μs chirp has a 1.5 km dead zone even though its compressed range resolution may be a few meters. For this reason multifunction radars interleave a short-pulse, high-pulse-repetition-frequency waveform to fill the near range, accepting reduced energy on those returns because nearby targets are strong anyway.
The optical analogue is the OTDR. A reflectometer fires an optical pulse into a fiber and times the Rayleigh backscatter. The Fresnel reflection from the launch connector is many orders of magnitude stronger than the backscatter and saturates the photodiode, so the receiver needs recovery time before it can resolve weak signal again. The result is an attenuation dead zone of a few meters and a shorter event dead zone over which two reflective features cannot be separated. Both scale with pulse width, and both are pushed off the fiber under test by inserting a launch fiber or a pulse suppressor.
Governing Relationships
Rmin = c × τ / 2 ≈ 150 m per μs of pulse width
OTDR dead-zone distance:
d = vg × τ / 2 = c × τ / (2 ng) ≈ 0.1 m per ns (ng ≈ 1.468)
MTI blind speeds (velocity dead zone):
vblind = n × λ × PRF / 2 (n = 1, 2, 3, …)
Where c = 3 × 108 m/s, τ = pulse width, vg = group velocity, ng = fiber group index, λ = wavelength, PRF = pulse repetition frequency. Example: X band (λ = 3 cm) at PRF = 2 kHz → first blind speed = 30 m/s.
Dead Zone by System Type
| System | Dead zone | Root cause | Typical value | Mitigation |
|---|---|---|---|---|
| Pulsed radar | Near range Rmin | Receiver blanked during TX (eclipsing) | 15 m (100 ns) to 1.5 km (10 μs) | Short-pulse high-PRF fill waveform |
| FMCW radar | None inherent | Continuous wave, no TX/RX gating | ~0 m (TX/RX leakage limited) | Good TX/RX isolation |
| OTDR | Launch-end masking | Connector Fresnel reflection + detector recovery | 0.5 to 3 m event; 2 to 10 m atten. | Launch fiber, pulse suppressor |
| MTI radar | Velocity (blind speeds) | Doppler phase = multiple of 2π per pulse | n × 30 m/s at X band, 2 kHz PRF | PRF stagger, multiple PRFs |
| Bistatic radar | Baseline / forward-scatter | Direct-path masking near the TX-RX line | Geometry dependent | Multistatic geometry, gating |
Frequently Asked Questions
How do you calculate the minimum range of a pulsed radar?
The monostatic minimum range is Rmin = cτ/2, where τ is the transmit pulse width; the factor of two is the round trip. A 1 μs pulse gives 150 m of dead zone, a 100 ns pulse gives 15 m. Add the receiver and T/R limiter recovery time. With pulse compression the dead zone is still set by the uncompressed transmit pulse, which is why short-range modes use short pulses or a separate high-PRF waveform.
What causes the dead zone in an OTDR measurement?
The strong Fresnel reflection from the launch connector saturates the photodetector, which then needs recovery time before it can resolve weak Rayleigh backscatter. The event dead zone (separating two reflections) is typically 0.5 to 3 m and the attenuation dead zone is 2 to 10 m, both scaling with pulse width. Because d = cτ/(2ng), each nanosecond maps to about 0.1 m of fiber. A launch fiber moves connector events out of the dead zone.
How does MTI radar create a velocity dead zone, and how is it removed?
An MTI processor subtracts successive pulses to cancel clutter, which also cancels any target whose Doppler phase shift between pulses is a multiple of 2π. These blind speeds fall at vblind = nλPRF/2; at X band with a 2 kHz PRF the first is 30 m/s and every multiple is also blind. Staggering the PRF moves the blind speeds to the least common multiple of the individual PRFs, pushing the first effective notch far higher.