
A practical primer on phased array beam steering, scan loss, grating lobes, and why hybrid architectures are winning in modern ground terminals.
Ian Cleary
If you work in satellite communications, phased arrays are no longer a "future technology." They're shipping in ground terminals, LEO user equipment, and hybrid antenna products today. But the jump from parabolic dishes to phased arrays introduces a set of tradeoffs that aren't always intuitive — even for experienced RF engineers.
This post covers the fundamentals that matter most in practice: beam steering, scan loss, grating lobes, and the architectural choices between analog, digital, and hybrid beamforming.
A parabolic dish points mechanically. It has one beam, it's slow to reposition, and it can only track one satellite at a time. For GEO, that's fine — the satellite doesn't move relative to the ground.
For LEO and MEO constellations, everything changes:
The cost? Complexity. A 256-element phased array has 256 phase shifters, potentially 256 amplifiers, and a beamforming network that must be calibrated and controlled in real time.
Each element in a phased array receives a progressive phase shift to steer the beam. For a uniform linear array (ULA) with element spacing , the phase increment between adjacent elements to steer to angle from broadside is:
This is the fundamental equation. Everything else — scan loss, grating lobes, sidelobe levels — flows from it.
Key intuition: You're not moving the antenna. You're constructively interfering in the desired direction by making the wavefront from each element arrive in phase at the far field.
As you steer away from broadside, two things happen:
The combined effect is typically to in power, depending on the element design. At 60° scan, you've lost 3–6 dB of gain compared to broadside.
Practical implication: System designers must account for scan loss in the link budget at the worst-case scan angle. For a LEO terminal that needs to track down to 20° elevation, you're scanning to 70° from broadside — and the array is barely functional. Most systems set a minimum elevation angle of 30–40° to keep scan loss manageable.
Grating lobes appear when the element spacing exceeds a critical threshold. For scan angle , the grating lobe condition is:
At broadside only (), the limit is . For ±60° scan, it tightens to .
Why this matters: Grating lobes are full-power copies of the main beam. They cause interference to adjacent satellites, violate regulatory EIRP density masks, and waste transmit power. You can't "window" them away like sidelobes — they're a spatial aliasing artifact.
Design tension: Smaller spacing means more elements per unit area (higher cost, more power, more complexity) but cleaner patterns. The half-wavelength rule () is the standard compromise for arrays that need wide scan.
Uniform illumination gives the highest directivity but the worst sidelobes (−13.2 dB for a ULA). Amplitude tapering reduces sidelobes at the cost of directivity and beamwidth:
| Taper | First Sidelobe | Beamwidth Factor | Directivity Loss |
|---|---|---|---|
| Uniform | −13.2 dB | 1.0× | 0 dB |
| Cosine | −23 dB | 1.36× | 0.91 dB |
| Hamming | −42.8 dB | 1.36× | 1.34 dB |
| Taylor (−30 dB, ) | −30 dB | 1.14× | 0.46 dB |
| Chebyshev (−30 dB) | −30 dB | 1.12× | 0.42 dB |
Taylor and Chebyshev are the workhorses for satellite antennas because they let you specify the sidelobe level directly while keeping beamwidth growth small. Taylor tapers are preferred when you need low close-in sidelobes but can tolerate higher far-out sidelobes (common for regulatory compliance).
This is where architecture decisions get expensive.
Each element has a phase shifter (and optionally a variable gain amplifier), and signals are combined in the RF domain before a single ADC/DAC chain.
Every element has its own full RF chain (LNA → mixer → ADC or DAC → mixer → PA). Beamforming happens in the digital domain.
Subarrays of elements share analog beamforming, with digital combining across subarrays. A 256-element array might have 16 subarrays of 16 elements each, requiring only 16 RF chains.
The industry trend is hybrid. Pure digital is too expensive for commercial ground terminals. Pure analog can't support the multi-beam requirements of LEO constellations. Hybrid gives you 80% of digital's capability at 20% of the cost.
A phased array is only as good as its calibration. Manufacturing tolerances, temperature drift, mutual coupling, and component aging all introduce phase and amplitude errors that degrade the beam pattern.
What goes wrong without calibration:
Calibration approaches:
For fielded systems, OTA calibration on a regular schedule (daily or per-session) is standard practice.
When you replace a parabolic dish with a phased array in a link budget, several line items change:
The net result: a phased array often has 3–6 dB less peak performance than an equivalently-sized dish, but its ability to form multiple beams, steer electronically, and maintain links during handoff makes it the right choice for LEO/MEO ground terminals.
| Concept | Key Number | Why It Matters |
|---|---|---|
| Scan loss | 3–6 dB at 60° | Sets minimum elevation angle |
| Grating lobe limit | Drives element count and cost | |
| Half-wave spacing | Standard design rule for wide scan | |
| Taylor taper | −30 dB SLL, 0.46 dB loss | Best sidelobe/directivity tradeoff |
| Hybrid subarrays | 16–64 RF chains | Sweet spot for commercial terminals |
Phased arrays aren't magic — they're engineering tradeoffs with well-understood physics. The art is in choosing the right architecture for your link budget, regulatory constraints, and cost target.