ECE 521E — Radar & Satellite Engineering • 5th Year BSc. Electrical & Communication Engineering
Masinde Muliro University of Science and Technology (MMUST)
By the end of this unit, the student should be able to:
Prerequisites: Unit on Continuous Wave (CW) radar; signals & systems (Fourier analysis, sampling); communication systems (mixing, PLLs).
A plain CW radar transmits a pure tone and measures only the Doppler shift — it has no way to tell how far the target is, because the echo delay hides inside an unobservable constant phase. Frequency-modulated CW (FMCW) radar solves this by sweeping the transmitted frequency in a known pattern. The echo, delayed by td = 2R/c, is then a time-shifted copy of the sweep; at any instant the receiver sees a frequency difference between what is being transmitted now and what was transmitted when the echo left. This difference — the beat frequency fb — is proportional to delay, and hence to range.
| Attribute | Unmodulated CW | FMCW | Pulsed |
|---|---|---|---|
| Range | ✗ Not possible | ✔ Beat frequency | ✔ Pulse delay |
| Velocity | ✔ Doppler | ✔ Doppler / ramp difference | ✔ (MTI needed) |
| Peak power | Low | Low | Very high |
| Minimum range | None | None | cτ/2 (eclipsing) |
| Hardware cost | Low | Moderate (linear sweep) | High (peak power) |
| Typical domain | Speed guns | Automotive, altimeters, level | Long-range surveillance |
The choice of frequency modulation pattern determines what can be measured and how cleanly. Four waveforms dominate practice:
Linear ramp, reset, repeat. Simplest to generate; beat frequency directly gives range. Moving targets smear the single-ramp beat (range–Doppler coupling), so automotive radars use multiple interleaved ramps instead of a pure sawtooth.
Up-ramp + down-ramp pair. Doppler shifts the beat oppositely on the two ramps, enabling clean separation of range and velocity from two measurements — the classical decoupling technique.
Hops between two discrete frequencies. Range from the phase difference between echoes at the two tones; very simple processing, but limited unambiguous range and no fine resolution.
Synthesizer steps through N frequencies; inverse FFT of the received phasors gives a high-resolution range profile. Excellent bandwidth control (DDS), at the cost of longer measurement time.
Let the transmitted frequency ramp linearly from f0 to f0+B over sweep time Tm. The instantaneous transmitted frequency and phase are:
The echo from a target at range R arrives after delay td = 2R/c, and (if the target moves) carries a Doppler shift fd = 2vr/λ:
The receiver mixes the echo with a sample of the transmitted signal; the difference term of the product cos(φTX)·cos(φRX) contains the phase difference Δφ = φTX − φRX. A low-pass filter removes the sum term, leaving:
For stationary or slow targets, the Doppler term is negligible or lumped into a range error, giving the working equation:
With a triangular waveform, the ramp slope reverses on the down-leg. The Doppler shift fd keeps the same sign on both legs (it depends on motion, not on the sweep direction), while the range-induced beat changes sign with the slope:
Adding and subtracting the two measured beats recovers both quantities:
Equivalently, fd = (fdown − fup)/2 and vr = fdλ/2.
Rather than one up/down pair, automotive radars transmit a frame of N chirps with slightly different slopes (a chirp sequence). Range comes from the beat frequency (fast-time FFT); velocity comes from the phase progression of the beat across the chirp sequence (slow-time FFT — the same Doppler-FFT idea as pulsed radar, with chirps playing the role of pulses). This 2-D processing cleanly separates range and Doppler and resolves multiple targets.
Set purely by sweep bandwidth — identical to the pulsed-radar result (B ≈ 1/τ). A 4 GHz sweep gives 3.75 cm resolution; this is why automotive short-range radar uses multi-GHz chirps.
Beat frequencies above half the sampling rate fs alias (Nyquist). The maximum measurable beat, and hence range, is:
The fast-time observation window Tm sets the beat-frequency resolution Δfb = 1/Tm, which maps back to a range resolution — consistency with ΔR = c/2B requires B·Tm ≥ 1 (the time–bandwidth product must exceed unity).
where Tc is the chirp repetition interval and N the number of chirps in the frame. Short chirps give wide unambiguous velocity; long frames give fine velocity resolution — a direct echo of pulsed-radar PRF trade-offs.
| Requirement | Design lever |
|---|---|
| Fine range resolution | Large sweep bandwidth B |
| Long unambiguous range | Small slope B/Tm (long Tm for given B) |
| Large unambiguous velocity | Short chirp interval Tc |
| Fine velocity resolution | Long frame N·Tc |
| Multiple-target separation | 2-D range–Doppler processing (chirp sequence) |
The derivation in Section 3 assumes a perfectly linear frequency ramp. Real VCOs exhibit nonlinear tuning (S-curves, drift), which broadens and distorts the beat spectrum: instead of a single clean tone per target, the beat becomes a chirp-like smear, degrading resolution and detection.
| Method | Linearity | Complexity/Cost | Typical Use |
|---|---|---|---|
| VCO (voltage-controlled oscillator), free-running | Poor | Lowest | Simple proximity/level radar |
| PLL-linearized VCO | Good | Moderate | Automotive, altimeters |
| DDS-based chirp synthesis | Excellent | Moderate–High | Instrumentation, stepped chirp, radar-on-chip |
| Fractional-N PLL chirp modulator | Very good | Moderate | 77/79 GHz automotive radar ICs |
Because TX is always on, FMCW inherits the CW isolation problem — worsened by the fact that the near-field leakage from the TX antenna directly enters the mixer, producing a huge "zero-beat" DC component that can saturate the ADC. Mitigations: antenna separation, absorptive shielding, TX-leakage cancellation networks, and digital DC-offset removal. Monostatic (single-antenna) automotive radars rely on circulators/isolators with typically 20–30 dB of inherent isolation plus calibration.
Aircraft FMCW altimeters (C-band, ~4.3 GHz, B ≈ 100–165 MHz) give 0.5–1 m resolution from ~1,500 ft down to the runway — no minimum-range dead zone, low peak power. Spaceborne and planetary-lander altimetry uses related FM/chirp techniques for precision descent ranging.
26/60/80 GHz FMCW level radars measure tank and silo contents with millimetre accuracy, immune to dust, vapor and temperature — replacing ultrasonic and guided-wave devices in harsh process plants.
Low-power FMCW at 24/60 GHz supports perimeter intrusion detection, people counting, and vital-signs monitoring (chest-motion micro-Doppler at a few tens of cm).
Triangular-FMCW seekers provide passive-appearing ranging in air-to-air engagements; artillery proximity fuzes use FM ranging derivatives for height-of-burst control.
Ground-penetrating radar (GPR) and snow/ice thickness sounders frequently use stepped-FMCW or chirp waveforms to build high-resolution subsurface profiles.
An FMCW radar sweeps B = 200 MHz in Tm = 0.5 ms. The measured beat frequency is fb = 66.7 kHz. Find the target range and the range resolution.
R = c·Tm·fb/(2B) = (3×108 × 5×10−4 × 6.67×104)/(4×108) = 25 m.
ΔR = c/2B = 3×108/(4×108) = 0.75 m.
A 77 GHz automotive radar (λ ≈ 3.9 mm) uses a triangular waveform with B = 1 GHz, Tm = 1 ms per ramp. It measures fup = 380 kHz and fdown = 420 kHz. Find range and radial velocity.
R = c·Tm(fup+fdown)/(4B) = 3×108 × 10−3 × 8×105 / (4×109) = 60 m.
fd = (420 − 380)/2 = 20 kHz; vr = fdλ/2 = 2×104 × 3.9×10−3/2 ≈ 39 m/s (≈ 140 km/h).
The same 77 GHz radar transmits a frame of N = 128 chirps, each with repetition interval Tc = 40 μs. Find the maximum unambiguous velocity and the velocity resolution.
vmax = λ/(4Tc) = 3.9×10−3/(1.6×10−4) ≈ 24.4 m/s.
Δv = λ/(2NTc) = 3.9×10−3/(2 × 128 × 4×10−5) ≈ 0.38 m/s.
Range: — m
Range resolution: — m
Q1. State the two measurable quantities provided by a triangular-FMCW radar and the beat-frequency combinations that yield each.
Answer: Range: R = c·Tm(fup+fdown)/4B; Velocity: from fd = (fdown−fup)/2, vr = fdλ/2.
Q2. An FMCW radar sweeps 500 MHz in 2 ms and measures a beat of 25 kHz. Find the range.
Answer: R = 3×108×2×10−3×2.5×104/(109) = 15 m.
Q3. Explain range–Doppler coupling in a single-ramp FMCW waveform.
Answer: The measured beat fb = (B/Tm)(2R/c) + fd mixes range and velocity information; a moving target appears at an apparent range offset ΔR = c·Tm·fd/(2B) — indistinguishable from a range change without a second measurement.
Q4. What bandwidth gives 5 cm range resolution, and why?
Answer: B = c/(2ΔR) = 3×108/0.1 = 3 GHz; resolution depends only on bandwidth, not carrier.
Q5. Why does sweep nonlinearity degrade FMCW performance, and name two correction methods.
Answer: Nonlinear frequency-vs-time smears the beat tone into a chirp, broadening the spectral peak and degrading resolution/detection. Corrections: PLL-locked VCO, DDS chirp synthesis, reference-delay calibration, frequency-domain resampling (any two).
Q6. In chirp-sequence processing, which FFT gives range and which gives velocity?
Answer: Fast-time FFT (within each chirp) → range; slow-time FFT (across the N chirps per range bin) → Doppler/velocity.
Q7. A 79 GHz (λ = 3.8 mm) chirp-sequence radar uses Tc = 25 μs. Find vmax.
Answer: vmax = λ/(4Tc) = 3.8×10−3/10−4 = 38 m/s.
Q8. Give two reasons FMCW suits planetary landing radar compared with pulsed radar.
Answer: Low peak power (power-limited lander) and no minimum-range dead zone (needed in final descent metres); also continuous measurement of altitude/rate (any two).
Q9. What sets the maximum unambiguous range in an FMCW system?
Answer: The ADC sampling rate: fb must stay below fs/2 (Nyquist), so Rmax = c·Tm·fs/(4B).
Q10. A triangular-FMCW radar with λ = 3 cm, B = 150 MHz, Tm = 1 ms measures fup = 45 kHz, fdown = 55 kHz. Find R and vr.
Answer: R = 3×108×10−3×105/(6×108) = 50 m; fd = 5 kHz; vr = 5000×0.03/2 = 75 m/s.