Title: Ray Tracing
1Ray Tracing
A radio signal will typically encounter multiple
objects and will be reflected, diffracted, or
scattered These are called multipath signal
components
2- Represent wavefronts as simple particle
- Geometry determines received signal from each
signal component - Typically includes reflected rays, can also
include scattered and diffracted rays - Requires site parameters
- Geometry
- Dielectric properties
- Error is smallest when the receiver is many
wavelengths from the nearest scatterer and when
all the scatterers are large relative to a
wavelength
3- Accurate model under these conditions
- Rural areas
- City streets when the TX and RX are close to the
ground - Indoor environments with adjusted diffraction
coefficients - If the TX, RX, and reflectors are all immobile,
characteristics are fixed - Otherwise, statistical models must be used
4Two Ray Model
Used when a single ground reflection dominates
the multipath effects.
- Approach
- Use the free space propagation model on each
ray - Apply superposition to find the result
5time delay of the ground reflection relative to
the LOS ray
product of the transmit and receive antenna field
radiation patterns in the LOS direction
6product of the transmit and receive antenna field
radiation patterns corresponding to x and x,
respectively
R Ground reflection coefficient
7Delay spread delay between the LOS ray and the
reflected ray
8If the transmitted signal is narrowband wrt the
delay spread
9phase difference between the two received signal
components
10d Antenna separation h t Transmitter height h
r Receiver height
11When d is large compared to h t h r
Expand into a Taylor series
12The ground reflection coefficient is given by
vertical polarization
horizontal polarization
for ground, pavement, etc...
13For very large d
14- As d increases, the received power
- Varies inversely with d 4
- Independent of ?
15f 900 MHz R - 1 h t 50 m h r 2 m
G l 1 G r 1 P t 0 dBm
16- The path can be divided into three segments
- d lt h t
- The two rays add constructively
- Path loss is slowly increasing
17- h t lt d c
- Wave experiences constructive and destructive
interference - Small scale (Multipath) fading
- If power is averaged in this area, the result is
a piecewise linear approximation
- d c lt d
- Signal power falls off by d 4
- Signal components only combine destructively
18To find d c , set
- In segment 1, d lt h t power falls off by
- In segment 2, h t lt d lt d c power falls off by
20 db/decade - In segment 3, d c lt d, power falls off by 40
db/decade - Cell sizes are typically much less than d c and
power falls off by
19Problem 2 5
Find the critical distance, d c , under the two
ray model for a large macrocell in a suburban
area with the base station mounted on a tower or
building (h t 20 m), the receivers at height h
r 3 m, and f c 2 GHz. Is this a good size
for cell radius in a suburban macrocell? Why or
why not?
Solution
20Ten Ray Model (Dielectric Canyon)
- Assumptions
- Rectilinear streets
- Buildings along both sides of the street
- Transmitter and receiver heights close to street
level - 10 rays incorporate all paths with 1, 2, or 3
reflections - LOS (line of sight)
- GR (ground reflected)
- SW (single wall reflected)
- DW (double wall reflected
- TW (triple wall reflected)
- WG (wall ground reflected)
- GW (ground wall reflected)
21Overhead view of 10 ray model
x i path length of the i th reflected ray
Product of the transmit and receive antenna gains
of the i th ray
22Assume a narrowband model such that
for all i
- Power falloff is proportional to d - 2
- Multipath rays dominate over the ground reflected
rays that decay proportional to d - 4
23General Ray Tracing
- Models all signal components
- Reflections
- Scattering
- Diffraction
- Requires detailed geometry and dielectric
- properties of site
- Site specific
- Similar to Maxwell, but easier math
- Computer packages often used
- The GRT method uses geometrical optics to trace
the propagation of the LOS and reflected signal
components
24Shadowing Diffraction and Spreading
Diffraction
- Diffraction occurs when the transmitted signal
"bends around" an object in its path
- Most common model uses a wedge which is
asymptotically thin - Fresnel knife edge diffraction model
25For h small wrt d and d', the signal must travel
an additional distance ? d
The phase shift is
26is called the Fresnel Kirchhoff diffraction
parameter
Approximations for the path loss relative to LOS
are
27Scattering
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29- Okumura model
- Empirically based (site/freq specific)
- Awkward (uses graphs)
- Hata model
- Analytical approximation to Okumura model
- Cost 136 Model
- Extends Hata model to higher frequency (2 GHz)
- Walfish/Bertoni
- Cost 136 extension to include diffraction from
rooftops
30Simplified Path Loss Model
K dimensionless constant that depends on the
antenna characteristics and the average channel
attenuation d 0 reference distance for the
antenna far field ? path loss exponent
LOS, 2 ray model, Hata model, and the COST
extension all have this basic form
31Generally valid where d gt d 0 d 0 1 10 m
indoors 10 100 m outdoors
- General approach
- Take data at three values of d
- Solve for K, d o , and ?
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