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ISART '99 Boulder, Sept. 8-10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at Austin [email protected] George H. Hagn SRI International [email protected]

Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

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Page 1: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 1

Effects of Trees on Slant Propagation Paths

Wolfhard J VogelThe University of Texas at Austin

[email protected]

George H. HagnSRI International

[email protected]

Page 2: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 2

Content

• Terrestrial vs. Satellite Tree Attenuation

• VHF, UHF, L-Band, S-Band and K-Band Measurements and Model Comparison

• Foliage Effects Scaling

• Spatial, Frequency, Elevation Variations

• Conclusions

Page 3: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 3

Paths and Models

Horizontal: long Slant: med. Roadside: short

TX RX TX

RX

SLAB Model SLAB Model Physical or Empirical

Page 4: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 4

Horizontal Path Tree Attenuation

• Absorption, Scattering, Lateral wave over tree boundary layer, Slab model for layers, e.g., undergrowth, trunks, crowns

• Long propagation path through many trees

• Below 3° in elevation

• High initial specific attenuation, R

Ø 2-10 dB/m

• Fade, A = increase diminishes with range, d

))exp(1(max

max A

dRAA

⋅−−=

Page 5: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 5

Slant Path Tree Attenuation

• Short propagation path through 1 or 2 trees

• Absorption, Scattering, Ground reflection

• Usually above 10° in elevation

• Fade = attenuation constant * path length

Page 6: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 6

VHF Measurements

• Vegetation– Eucalyptus Forest (California)– Tropical Rain Forest (Asia)

• Frequencies - 50, 75, 100, 250, 400 MHz• Polarization – linear, V and H • Platforms - aircraft towed & balloon borne• Elevation Angles – 8° to 29°• Calibration - Relative, by (1) differential path

lengths at forest edge, (2) measured or (3) calculated clear path comparison

Page 7: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 7

VHF Results

0.075 – 0.200V400

0.076 – 0.146H400

0.054 – 0.108V250

0.040 – 0.075H250

0.145 – 0.1510.075 – 0.1400.043 - 0.120V100

0.061 – 0.1330.030 – 0.0700.048 - 0.100H100

0.075 – 0.1250.043 - 0.090V75

0.075 – 0.1100.038 - 0.075H75

0.060 – 0.1000.070 – 0.1200.045 - 0.090V50

0.012 – 0.0300.040 - 0.1000.031 - 0.060H50

EucalyptusJungle BJungle A(V/H)(MHz)

Median Attenuation Constant (dB/m)Pol.Freq.

Page 8: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 8

Comparison to Frequency Scaling Model

Solid line: Model with 1dB/m at 1 GHz

Red symbols: H Pol.

Blue symbols: V Pol.

⋅=

5.0

2

5.0

112

11exp)()(

ffbfAfA

100200 300 400 500908070605040

Frequency (MHz)

0.01

0.1

1

Fo

rest

Att

enu

atio

n (

dB

/m)

b =1.173 for median fade level

Page 9: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 9

Comments to VHF Results

• Due to tree morphology, vertical polarization fades more than horizontal polarization

• Model under-predicts attenuation to 100 MHz– Model is based on UHF to K-Band measurements

• Model over-predicts attenuation at 250 and 400 MHz– Paths were longer than 5 – 10 m, above which the

effective specific attenuation decreases

• Model could be tuned to reflect VHF measurements

Page 10: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 10

UHF (870 MHz, CP) Measurementsof Single TreesAttenuation (dB) Attenuation Coefficient (dB/m)

Tree Type Largest Average Largest Average

Burr Oak* 13.9 11.1 1.0 0.8

Callery Pear 18.4 10.6 1.7 1.0

Holly* 19.9 12.1 2.3 1.2

Norway Maple 10.8 10.0 3.5 3.2

Pin Oak 8.4 6.3 0.85 0.6

Pin Oak* 18.4 13.1 1.85 1.3

Pine Grove 17.2 15.4 1.3 1.1

Sassafras 16.1 9.8 3.2 1.9

Scotch Pine 7.7 6.6 0.9 0.7

White Pine* 12.1 10.6 1.5 1.2

Average 14.3 10.6 1.8 1.3

RMS 4.15 2.6 0.9 0.7

Page 11: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 11

L-Band (1.6 GHz, CP) Measurementsof Single Trees

T r e e T y p e A v e r a g e

A t t e n u a t i o n ( d B )

A t t e n u a t i o n C o e f f i c i e n t

( d B / m )

W i l lo w 1 0 . 4 5 1 . 1

P i n e 1 8 . 0 1 . 8

L i n d e n 9 . 1 1 . 4

E u r o p e a n A l d e r 7 . 0 1 . 0

A c a c i a 6 . 7 5 0 . 9

P o p la r 3 . 5 0 . 7

E lm 9 . 0 1 . 2

H a z e l n u t 2 . 7 5 1 . 1

M a p l e 1 6 . 2 5 1 . 2 5

W h i t e S p r u c e 2 0 . 1 1 . 7 5

L a u r e l C h e r r y 1 2 . 0 2 . 0

P l a n e 1 6 . 9 1 . 3 5

F i r 1 2 . 7 5 1 . 5

F r u i t 9 . 6 1 . 2

A v e r a g e 1 1 . 0 1 . 3

R M S 5 . 1 0 . 3 5

Page 12: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 12

Signal Variation with Position

Edge of Tree

(CP)

No 1:1 frequency correlation due to scattering

Page 13: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 13

Simultaneous L- and S-Band Measurementsof Single Trees VS Position

PecanCottonwood Pine

Large variations with positiondue to scattering

weak frequency dependence

L

L

LS S

S

Page 14: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 14

Signal Variation with FrequencyPine Tree; 5, 10, 15, 20 dB average fade

160 MHz

Short delay times of mostly forward scattered waves

Relatively flat fading

Page 15: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 15

2 GHz MeasurementsDeciduous tree grove, TDRSS, CP

WestEast

South

Measurement 1Measurement 2(2 weeks later)

TDRS-1 was drifting East

TDRS-7 was fixed

Page 16: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 16

Tree Grove Fading at 2 GHz (TDRSS)Elevation Angle Dependence, 24° vs 41° and 49°

-5 0 5 10 15 20 25 30Fade (dB)

2

3

4

56789

2

3

4

56789

1

10

100

Pro

bab

ility

th

at F

ade

> A

bsc

issa

(%

)

T7, T1 Independent

T1 (41°, 49° el)

T7 (24° el)

Max(T7,T1)Diversity

Page 17: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 17

Comments to 2 GHz TDRSS Data

• CDFs for T7 at 24° repeated to within 0.5 dB rms

• CDFs for T1 at 49° and later at 41° are almost identical– for a layer of uniform-height vegetation

– if attenuation proportional to path length in the medium

– fading at 41° should be 87% of fading at 49°

• Loo Model for tree shadowing

°°==°° 49sin/24sin54.0/ 2449 µµ

2

2

02

)log20(exp[

12686.8)(

σ

µ

πσ

−= ∫

∞z

z

KxxpLoo

- ratio of means agrees with layer model

Page 18: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 18

K-Band MeasurementsRoadside Trees in Maryland

0 5 10 15 20 25 30 35 40 45

Fade Depth (dB)

1

10

100

2

3

4

56789

20

30

40

5060708090

Per

cen

tag

e o

f D

ista

nce

Fad

e >

Ab

scis

sa

ACTS Meas. (No Foliage)ACTS (Foliage Scaled)Helo Meas. (Freq. Scaled)EERSFoliage scaling of

fading in dB:

UHFAF=1.35* ANF

L-BandAF=2.33+0.9* ANF

K-Band58.08.635.0 NFF AA +=

Page 19: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 19

Frequency Scaling of Fade DistributionSingle Tree: Pecan in Leaf

0 5 10 15 20 25 30 35 40 45 50 55 60

Fade (dB)

1

10

100

2

3

4

56789

20

30

40

5060708090P

erce

nta

ge

of

Dis

tan

ce >

Ab

scis

sa

L-Band Measurement K-Band Measurement

Scaling Model

⋅=

5.0

2

5.0

112

11exp)()(

ffbfAfA

With b =1.5scales best below ~30%

Page 20: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 20

Frequency Scaling for Median FadeValid for Trees with Foliage, b=1.173

No Foliage

100 1000 10000

200

400

600

800

2000

4000

6000

8000

2000

0806040

Frequency (MHz)

0

1

2

3

4

5

Sp

ecif

ic T

ree

Att

enu

atio

n (

dB

/m)

Page 21: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 21

Conclusions - 1• Average short path multi-tree attenuation at

– VHF (100 MHz) is 0.03 to 0.15 dB/m– VHF (400 MHz) is 0.075 to 0.2 dB/m

• Average single tree attenuation at– UHF (870 MHz) is 10.6 dB (2.6 dB RMS) – L-Band (1.6 GHz) is 11 dB (5.1 dB RMS)– K-Band (20 GHz) is 23 dB

• The frequency scaling formulation pertaining to trees in full foliage at frequencies between VHF (25 MHz) and K-Band (20 GHz) is given by

where A(f1 ), A(f2 ) are the respective equal probability attenuations (dB) at frequencies f1, f2 (in GHz), with b=1.173 for median, b=1.5 for 1% to 30% of distribution.

⋅=

5.0

2

5.0

112

11exp)()(

ffbfAfA

Page 22: Effects of Trees on Slant Propagation Paths - …...ISART '99 Boulder , Sept. 8 -10, 1999 1 Effects of Trees on Slant Propagation Paths Wolfhard J Vogel The University of Texas at

ISART '99 Boulder, Sept. 8-10, 1999 22

Conclusions - 2

• The dominant contributor to attenuation is the wood part of the tree at frequencies between VHF (50 MHz) and S-Band (4 GHz). For example, foliage has been found to introduce approximately 35% additional attenuation at UHF and 15% at L-Band

• At K-Band (20 GHz), the wood and leaf parts of the tree are both important showing increases due to foliage ranging from 2 to 3 times the attenuation

• As most signal variations in the shadow of a tree are due to forward scattering effects, the delays associated with the multipath are short and the fading is flat.