COST 231 Walfish-Ikegami
How the Walfish-Ikegami Model Estimates Urban Loss
The model emerged from the European COST 231 research action of the early 1990s, which combined the rooftop-diffraction theory of Walfisch and Bertoni with the street-level scattering work of Ikegami. It splits the propagation problem into a line-of-sight (LOS) street-canyon case and a non-line-of-sight (NLOS) case. In the LOS branch, when the mobile and base antenna can see each other down a street, a two-parameter formula based on Stockholm measurements applies. The far more common NLOS branch treats the signal as a wave that propagates over the rooftops by multiple forward diffraction across building rows, then diffracts down from the last rooftop edge into the street where the mobile sits.
The NLOS total loss is the sum of three components: ordinary free-space loss L0, the rooftop-to-street diffraction and scatter loss Lrts, and the multiscreen diffraction loss Lmsd. The Lrts term depends on street width w, the height difference between the rooftop and the mobile, and a street-orientation correction that accounts for whether the street runs toward or across the base station. The Lmsd term is the most involved: it models the cumulative diffraction over a series of equally spaced building screens and changes form depending on whether the base antenna is above, level with, or below the average rooftop height hroof.
Because Lrts and Lmsd can individually go negative under favorable geometry, the model clamps their sum at zero; when Lrts + Lmsd ≤ 0 the prediction reverts to pure free-space loss. This guard prevents the unphysical result of urban clutter improving the signal relative to free space, and it is one of the practical details engineers must implement carefully when coding the model into a planning tool.
Governing Equations
LLOS = 42.6 + 26·log10(d) + 20·log10(f) dB
Non-line-of-sight total loss:
LNLOS = L0 + Lrts + Lmsd (when Lrts + Lmsd > 0)
LNLOS = L0 (when Lrts + Lmsd ≤ 0)
Free-space term:
L0 = 32.4 + 20·log10(d) + 20·log10(f) dB
Rooftop-to-street diffraction:
Lrts = −16.9 − 10·log10(w) + 10·log10(f) + 20·log10(Δhmobile) + Lori
Where d = distance in km, f = frequency in MHz, w = street width in m, Δhmobile = hroof − hmobile, and Lori is the street-orientation correction (range −10 to +4 dB). Example: f = 900 MHz, d = 1 km, w = 25 m, hroof = 30 m, hbase = 12 m (base below rooftop), with b = 50 m typically yields a total NLOS loss near 160 dB (about 150 dB for a street running toward the base, rising to roughly 165 dB for a perpendicular street).
Geometry Inputs and Typical Values
| Input Parameter | Symbol | Typical Range | Role in Model |
|---|---|---|---|
| Frequency | f | 800 to 2000 MHz | Sets free-space and diffraction loss slope |
| Base antenna height | hbase | 4 to 50 m | Selects above/below-rooftop Lmsd branch |
| Mobile height | hmobile | 1 to 3 m | Drives rooftop-to-street drop Δh |
| Average building height | hroof | 9 to 50 m | Defines rooftop diffraction edge |
| Building separation | b | 20 to 50 m | Number of multiscreen diffractions |
| Street width | w | b/2 (typ. 10 to 25 m) | Sets Lrts magnitude |
| Street orientation | φ | 0° to 90° | Orientation correction Lori |
Frequently Asked Questions
What is the valid frequency and distance range for the COST 231 Walfish-Ikegami model?
The model is defined for 800 MHz to 2000 MHz, base antenna heights of 4 to 50 m, mobile heights of 1 to 3 m, and distances of 0.02 km to 5 km. It was calibrated on COST 231 measurements in European cities, so it is most accurate for dense and medium-density urban grids with fairly uniform building heights. Below 20 m, beyond 5 km, or into the millimeter-wave bands, the multiscreen diffraction terms lose validity and ray-tracing is preferred.
How does the model differentiate between line-of-sight and non-line-of-sight conditions?
For an LOS street canyon with the base below rooftop level it uses L = 42.6 + 26·log10(d) + 20·log10(f), valid for d ≥ 20 m. For NLOS the loss is L0 + Lrts + Lmsd; when Lrts + Lmsd ≤ 0 the model reverts to free-space loss alone. The LOS branch is empirical while the NLOS branch is built on Walfisch-Bertoni multiscreen diffraction physics.
What is the difference between the Walfish-Ikegami model and the Okumura-Hata model?
Okumura-Hata is fully empirical, using only frequency, antenna heights, and distance with a coarse clutter correction, and is defined down to about 1 km. Walfish-Ikegami adds explicit building geometry (height, separation, street width, orientation) and a physical rooftop diffraction mechanism, letting it model microcells with antennas below rooftop level down to 20 m. The trade-off is that it needs detailed morphology data Hata does not require.