Wireless Fading channel : Clarke's Model
A. One-Ring Diagram Exploration
Static View:
- Identify Tx (center red), Scatterers (red on ring), Rx (blue).
Change Number of Paths (K):
- Use the slider to vary K (e.g., min, mid, max).
- Observe scatterer count updates immediately without needing to click "Update Simulation".
Animate Rx Movement:
- Set Mobile Velocity (e.g., 10–20 m/s), click Start Animation.
- Watch the Rx (blue circle) move along the ring with an orange velocity vector.
- Change velocity during animation to see the speed effect.
- Click Stop Animation to end.
- Note: Animation is visual only; it doesn't affect charts unless "Update Simulation" is clicked.
B. Autocorrelation Function (R₀[n])
After each change, click Update Simulation to refresh the plot.
Amplitude (a):
- Higher
a
increases the peak atn=0
. - The overall shape and width of the main lobe remain mostly the same.
- Higher
Doppler Spread (Dᵥ):
- Increasing Dᵥ narrows the main lobe → faster decorrelation (shorter coherence time).
Bandwidth (W):
- Increasing W → slower decay of R₀[n] (wider main lobe).
- Related to J₀ argument:
nπDᵥ/W
.
Number of Samples:
- Affects x-axis range (length of the plot), not the core shape of R₀[n].
C. Doppler Power Spectrum (S(f))
After each change, click Update Simulation to refresh the plot.
Default Shape:
- Observe the characteristic “U-shape” or “bathtub” spectrum with edge peaks.
Amplitude (a):
- Changes the y-axis scale (overall power).
- Spectrum shape and frequency extent remain unchanged.
Doppler Spread (Dᵥ):
- Wider Dᵥ → broader frequency range.
- Non-zero values for
|f| ≤ Dᵥ/(2W)
.
Bandwidth (W):
- Increasing W → narrower spectrum range.
- Inversely proportional to frequency spread (
Dᵥ/2W
).
Number of Samples:
- Higher sample count → smoother, more detailed plot.
D. Additional Parameters
Coherence Time Factor:
- Vary it and observe if there's any effect.
- It may not directly affect R₀[n] or S(f) in this version.
Number of Paths (K):
- Affects only the One-Ring Diagram.
- Higher K better approximates the ideal infinite-scatterer assumption in Clarke’s model.