Abstract
Recently there has been a significant amount of interest in the area of wideband
and ultra-wideband (UWB) signaling for use in indoor wireless systems. This interest is
in part motivated by the notion that the use of large bandwidth signals makes systems less
sensitive to the degrading effects of multipath propagation. By reducing the sensitivity to
multipath, more robust and higher capacity systems can be realized. However, as signal
bandwidth is increased, the complexity of a Rake receiver (or other receiver structure)
required to capture the available power also increases. In addition, accurate channel
estimation is required to realize this performance, which becomes increasingly difficult as
energy is dispersed among more multipath components.
In this thesis we quantify the channel response for six signal bandwidths ranging
from continuous wave (CW) to 1 GHz transmission bandwidths. We present large scale
and small scale fading statistics for both LOS and NLOS indoor channels based on an
indoor measurement campaign conducted in Durham Hall at Virginia Tech. Using newly
developed antenna positioning equipment we also quantify the spatial correlation of these
signals. It is shown that the incremental performance gains due to reduced fading of
large bandwidths level off as signals approach UWB bandwidths. Furthermore, we
analyze the performance of Rake receivers for the different signal bandwidths and
compare their performance for binary phase modulation (BPSK). It is shown that the
receiver structure and performance is critical in realizing the reduced fading benefit of
large signal bandwidths. We show practical channel estimation degrades performance
more for larger bandwidths. We also demonstrate for a fixed finger Rake receiver there
is an optimal signal bandwidth beyond which increased signal bandwidth produces
degrading results.
Acknowledgments
At this time I would like to thank Michael Buehrer, William Davis, Jeffery Reed, and
Raqib Mostafa for serving on my advisory committee and providing technical expertise
as well as encouragement along the way. I would also like to acknowledge the Via
family for the generous endowment provided by the Harry Lynde Bradley Fellowship
which allowed me to pursue this research almost completely un-tethered from the reins.
I would also like to express my appreciation to my fellow graduate students in MPRG,
especailly Joseph Gaeddert, Chris Anderson, Brian Donlan, Vivek Bharadwaj, Aaron
Orndorf and John Keaveny for their thought provoking discussions and technical
assistance with this research. Also my appreciation goes to Samir Ginde, Carlos Aguayo,
Nathan Harter and my other lab mates for keeping things in perspective while working at
MPRG. Of the MPRG staff, which was extremely helpful, I would like to thank Mike
Hill, Shelby Smith, Hilda Reynolds, and Shereef Sayed.
I am greatly indebted to Mike Coyle and the staff of the Industrial Design Metal Shop for
their help in designing and manufacturing the antenna positioning system. Without
Mike’s support the positioning system would not have proceeded beyond the conceptual
stage. For donating replacement couplers for the positioning system I would like to thank
the staff at Ruland. I also owe thanks to Josiah Hernandez for helping with the
measurement campaign. I must also thank Dennis Sweeney from CWT and Carl Dietrich
from VTAG for their insight and use of their equipment during the measurement
campaign.
I owe a very special thanks to Alexander Taylor, who has been my partner in Electrical
Engineering crime for the past five years at Virginia Tech and has been an honest friend
through it all. Also the friendships forged with Aaron Orndorf and Jeremy Barry have
made this experience an interesting one to say the least.
Without a doubt none of this work would have been possible without the tireless support
and understanding of my fiancé and soon to be wife Ashley K. Rentz. Her
encouragement, wisdom, and unwavering love were instrumental in completing this
work; thank you for understanding.
Finally, I would like to thank my parents Bob and Louise Hibbard, as well as my brother
Mark Hibbard for their generous support, love, and understanding throughout this work
as well as my entire life.
Table of Contents
CHAPTER 1
INTRODUCTION AND THESIS OVERVIEW .1
1.1 Motivation 1
1.2 Background and Perspective . 2
1.3 Thesis Overview . 3
CHAPTER 2
RADIO WAVE PROPAGATION AND THE INDOOR PROPAGATION
CHANNEL 5
2.1 Introduction . 5
2.2 Propagation Overview . 6
2.2.1 Antennas and Radiation . 6
2.2.2 Propagation Mechanisms . 9
2.2.3 The Friis Transmission Formula and Basic Communication Link 14
2.3 The Indoor Propagation Channel . 17
2.3.1 Large Scale Effects 17
2.3.2 Small Scale Effects 19
2.4 Multipath Mitigation Techniques . 30
2.4.1 Basic Diversity Methods . 30
2.4.2 The Rake Receiver – An Overview . 31
2.5 Impact of Signal Bandwidth on Indoor Wireless Systems – Literature Review . 32
2.6 Summary 38
CHAPTER 3
SLIDING CORRELATOR CHANNEL MEASUREMENT: THEORY AND
APPLICATION 40
3.1 Introduction . 40
3.2 Overview of Channel Measurement Techniques . 40
3.3 Sliding Correlator Theory and Operation . 42
3.3.1 Cross Correlation Theory 42
v i
3.3.2 Pseudorandom Noise Sequences and Generators 44
3.3.3 Swept Time Delay Cross Correlation (Sliding Correlator) Theory . 46
3.3.4 Practical Considerations in the Sliding Correlator Measurement System . 51
3.4 Implementation of a Sliding Correlator Measurement System . 53
3.4.1 Transmitter and Receiver Implementation 53
3.4.2 System Calibration 56
3.4.3 System Repeatability . 58
3.5 Mapping Power Delay Profiles to Received Power . 59
3.6 Summary 61
CHAPTER 4
DESIGN AND IMPLEMENTATION OF AN ANTENNA POSITIONING AND
ACQUISITION SYSTEM .62
4.1 Introduction . 62
4.2 Positioning System Design Issues 62
4.2.1 Approaches to Antenna Positioning 63
4.2.2 Overall System Constraints . 64
4.2.3 Electrical Impact of Positioning System . 66
4.3 Positioning System Design and Implementation . 67
4.3.1 Design . 67
4.3.2 Implementation . 73
4.4 Antenna Positioning and Acquisition (APAC) Software 74
4.4.1 Defining the 2-D Measurement Grid . 75
4.4.2 Software Implementation Using Labview . 77
4.4.3 Additional Functionality 81
4.5 Positioning System Verification and Calibration 83
4.6 Conclusion 85
CHAPTER 5
INDOOR PROPAGATION MEASUREMENTS AND RESULTS AT 2.5 GHZ 86
5.1 Measurement Overview . 86
5.2 Measurement Campaign 86
5.2.1 Omnidirectional Biconical Antennas . 86
5.2.2 Narrowband (CW) Channel Sounder Configuration . 87
5.2.3 Wideband (Sliding Correlator) Channel Sounder Configuration 88
5.2.4 Measurement Procedure 90
5.2.5 Measurement Locations and Site Information . 91
vi i
5.3 Measurement Results and Processing 95
5.3.1 Large Scale Results . 95
5.3.2 Small Scale Results . 99
5.3.3 A Note on Site Specific Phenomena 118
5.4 Conclusion 121
CHAPTER 6
IMPACT OF SIGNAL BANDWIDTH ON INDOOR COMMUNICATION
SYSTEMS .122
6.1 Introduction . 122
6.2 Overview of BPSK Modulation and BER in AWGN 122
6.3 BER performance for BPSK in Measured Channels 124
6.4 Required Fading Margin for Quality of Service . 128
6.5 Spatial Correlation and Two Antenna Selection Diversity . 130
6.6 Rake Receiver Implementation and Channel Estimation . 132
6.6.1 Rake Receiver Performance – Perfect Channel Estimation . 133
6.6.2 Rake Receiver Performance – Imperfect Channel Estimation 134
6.6.3 Selective Rake Receiver Performance . 138
6.6.4 Selective Rake Receiver Performance with Channel Estimation 142
6.7 Conclusions 144
CHAPTER 7
CONCLUSIONS .145
7.1 Summary of Findings . 145
7.1.1 Impact of Spreading Bandwidth on Channel Characteristics 145
7.1.2 Impact of Spreading Bandwidth on DS-SS BPSK Indoor Systems 146
7.1.3 Original Contributions and Accomplishments 146
7.2 Further Areas of Research 147
7.2.1 On the Impact of Spreading Bandwidth 147
7.2.2 On the Use and Processing of Sliding Correlator Measurements 147
7.3 Closing 148
APPENDIX A
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A NA NA
400 26.6 22.6 0.9 8.8 22.2 20.2
Tx106
500 26.0 20.9 1.0 9.6 33.2 28.2
25 14.6 25.9 0.8 7.7 1.9 13.4
100 31.1 31.1 0.6 6.4 9.0 17.5
225 33.3 28.3 0.7 7.1 22.6 25.5
400 31.0 28.7 0.7 7.0 27.4 21.7
Tx107
500 31.1 31.0 0.6 6.5 31.7 21.3
25 11.9 22.3 0.9 9.0 2.2 17.4
100 34.6 31.2 0.6 6.4 11.0 20.4
225 35.8 32.9 0.6 6.1 17.4 14.6
400 32.2 26.6 0.8 7.5 34.8 27.8
Tx108
500 34.1 27.8 0.7 7.2 40.0 26.0
25 8.8 17.8 1.1 11.2 2.1 20.5
100 22.1 26.8 0.7 7.5 9.0 18.9
225 25.2 26.2 0.8 7.6 14.0 16.9
400 25.6 25.3 0.8 7.9 22.2 15.3
Tx109
500 23.4 23.4 0.9 8.5 24.0 17.0
160
Time Dispersion Parameters – Durham Hall 4th Floor – NLOS Measurements
(continued)
LOCATION SC TX
m (nsec)
RMS (nsec)
BC,90
(MHz)
BC,50
(MHz)
avg. number
of paths
Max Avg
SNR
(dB)
25 7.8 16.2 1.2 12.3 1.9 18.7
100 20.5 22.9 0.9 8.7 8.8 21.7
225 19.5 23.1 0.9 8.7 20.0 26.4
400 20.5 24.4 0.8 8.2 31.1 28.8
Tx110
500 20.4 23.8 0.8 8.4 33.8 26.7
25 7.1 17.4 1.1 11.5 2.1 21.8
100 25.8 29.3 0.7 6.8 9.7 18.9
225 29.3 32.0 0.6 6.3 19.4 18.8
400 28.9 29.7 0.7 6.7 28.2 21.5
Tx111
500 27.0 28.0 0.7 7.1 32.5 23.7
25 8.7 17.1 1.2 11.7 2.4 23.3
100 29.4 29.5 0.7 6.8 11.9 23.2
225 29.4 28.1 0.7 7.1 19.7 22.0
400 32.4 29.8 0.7 6.7 37.2 22.2
Tx112
500 33.0 29.1 0.7 6.9 31.0 16.7
25 7.7 15.7 1.3 12.7 2.25 22.8
100 25.4 26.9 0.7 7.4 11.0 22.6
225 16.6 17.5 1.1 11.4 9.6 15.2
400 30.0 25.5 0.8 7.8 36.1 23.1
Tx113
500 29.0 23.6 0.8 8.5 29.5 19.6
25 7.6 16.9 1.2 11.8 2.3 24.1
100 26.9 28.6 0.7 7.0 11.5 23.0
225 30.6 29.3 0.7 6.8 24.2 26.0
400 32.1 36.1 0.6 5.5 35.1 24.4
Tx114
500 31.6 31.5 0.6 6.3 36.8 23.5
25 9.9 18.7 1.1 10.7 2.4 22.7
100 29.2 30.3 0.7 6.6 10.9 20.7
225 29.2 31.1 0.6 6.4 26.5 27.0
400 29.3 30.1 0.7 6.6 33.4 25.5
Tx118
500 31.0 31.5 0.6 6.3 39.5 24.9
161
A.4 Probability of Error vs. Eb/No for BPSK Modulation
A.4.1 LOS Locations
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
LOS Rx000
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN Result
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
LOS Rx001
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN Result
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
LOS Rx002
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN Result
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
LOS Rx003
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN Result
162
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
LOS Rx004
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN Result
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
LOS Rx005
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN Result
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
LOS Rx006
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN Result
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
LOS Rx007
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN Result
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
LOS Rx008
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN Result
163
A.4.2 NLOS Locations
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx100
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx101
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx103
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx104
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx107
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
a
bi
lit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx108
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
164
b o
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx114
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx113
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx112
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx111
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx109
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
of
er
ro
r
Eb/No (dB)
NLOS Rx110
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
165
0 5 10 15
10-7
10-6
10-5
10-4
10-3
10-2
10-1
100
Pr
ob
ab
ilit
y
o
f e
rr
or
Eb/No (dB)
NLOS Rx118
Rayleigh Result
B = CW tone
B = 25 MHz
B = 100 MHz
B = 225 MHz
B = 400 MHz
B = 500 MHz
AWGN
166
Appendix B
Derivation of Instantaneous Wideband Received Power
in a 2 Path Fading Channel
This appendix shows in detail the derivation for instantaneous wideband received power.
We begin with the general result of the channel response to an arbitrary signal s(t) given
by
(1)
where the complex envelope notation is used without loss of generality. We consider the
case where s(t) is a repetitive pulse train p(t) with very narrow pulse width Tbb and
repetition period TREP which is much greater than the maximum measured excess delay of
the channel MAX. p(t) is defined as
(2)
From (1) we may write the response of the channel to the probing pulse as
(3)
To determine the instantaneous received power received at some time t0, the power
2
0 |)(~| tw is found by summing up the multipath powers resolved in the instantaneous
multipath power delay profile of the channel 20 |);(| τth . This is equal to the energy
received over the time duration of the multipath waveform, divided by the duration of the
waveform MAX [1]. Therefore the instantaneous received power at to is given by
)(
2
1)(~
1
0
k
j
k
k tpeatw k τ
θ
−=
=
kj
k
N
k
k eatshtshtstw
θττδττ ][
2
1)(~)(
2
1)(~)(~)(~)(~
1
0
−⊗=⊗=⊗=
−
=
bb
MAX
T
tp τ2)( = for 0 t Tbb
0)( =tp otherwise
167
(4)
(5)
(6)
Expanding the summations in (6) and applying Euler’s formula yields equation (7) as
(7)
Recombining the like terms of the first two terms in the integrand yields
(9)
Noting that integration is a linear operator, the integration is broken into two parts as
(9.1)
(9.2)
Recognizing the form of the autocorrelation of the sounding pulse in (9.2) we may
rewrite the result as
1 2
1 2
1 2
1 1
2
0 0 01 2
0 00
1 1| ( ) | ( ) ( ) ( ) ( )
4
MAX
k kj j
k k k k
k kMAX
w t a t e p t a t e p t dt
τ
θ θ
τ τ
τ
−
= =
= − −
∗
=
MAX
dttwtwtw
MAX
τ
τ 0
2
0 )(~)(~
1|)(~|
−−=
−
= =
MAX
kk dtetptptatatw jk
k
kk
k
k
MAX
τ
θθ
ττ
τ 0
)(1
0
10
1
0
01
2
0
21
2
1
2
2
)()()()(
4
11|)(~|
−+−=
MAX
tptatptatw
MAX
τ
ττ
τ 0
1
2
0
2
10
2
0
2
0
2
0 )()()()([4
1|)(~|
dttptptata )]()()cos()()(2 10100100 ττθθ −−−+
−=
=
MAX
k
kk
MAX
tptatw
τ
τ
τ 0
1
0
2
0
22 )()(
4
1|)(~|
)dttptptata )()()cos()()(2 10100100 ττθθ −−−+
=
−=
MAX
k
kk
MAX
dttptatw
τ
τ
τ 0
1
0
0
2
0
22 )()(
4
1|)(~|
dttptptata
MAX
MAX
−−−+
τ
ττθθ
τ 0
10100100 )()()cos()()(24
1
168
(10.1)
(10.2)
where Rp() is the autocorrelation of the sounding pulse given by
(11)
Note that while we defined p(t) in (2) the formulation of (10) is valid for any time limited
probing pulse. We will now consider the result of (10) for the pulse shape given by (2).
Substituting the definition of p(t) given by (2) into (10.1) and performing the integration
yields
(12)
Noting that the pulse is only defined over the range of times 0 t Tbb the result of the
integration is Tbb. Combining like terms in (12) yields
(13)
We next consider the second integral given by (10.2) of equation (10). Using the
definition of p(t) as a square pulse of width Tbb the autocorrelation function of (13) is
found by simple convolution , resulting in a triangular function [27] given by
(14)
−=
=
MAX
dttptatw k
k
k
MAX
τ
τ
τ 0
2
1
0
0
22
1 )()(4
1|)(~|
=
=
MAX
dt
T
ta
bb
MAX
k
k
MAX
τ
τ
τ 0
1
0
0
2 4)(
4
1
=
=
1
0
0
22
1 )(|)(~|
k
k tatw
=
−=
MAX
k
kk
MAX
dttptatw
τ
τ
τ 0
1
0
0
2
0
22 )()(
4
1|)(~|
)()cos()()(2
4
1
01100100 ττθθτ
−−+ p
MAX
Rtata
ζζττ dptpRp )()()(
0
−=
∞
=)(τpR
-Tbb 0
|| > Tbb
0 < Tbb
bb
MAX
T
τ4
+ 1
bbT
τ
+
− 1
bbT
τ
0
169
Combining equations (12), (13), and (14) yields the instantaneous received power t0 for
the two path channel as
(15)
where ak is the multipath amplitude, k is the multipath arrival time, k is the multipath
phase, and Rp() is the autocorrelation function given by equation (14).
)()cos()()(2)(|)(~| 01100100
1
0
0
22
0 ττθθ −−+=
=
p
k
k Rtatatatw
170
Appendix C
Antenna Positioning System User Guide and Reference
C.1 Introduction
This Appendix provides information concerning the use, maintenance, and
modification of the 4-bar parallel linkage antenna positioning system described in
Chapter 4. Care should be taken in operating the system as mechanical interference is
inherent in the design and no other mechanism other than operator awareness will prevent
serious or permanent damage to the equipment. It is very important that the user fully
understand the operating limitations of the positioning system as well as the stepper
motors before performing any positioning tasks. This appendix also contains trouble
shooting tips for repairing and maintaining the existing system, since at the time of
writing no document as such exists.
The scope of this system is limited to an indoor positioning system intended to
make measurements within the centimeter to millimeter wavelength band of the radio
spectrum in the interest of research. Therefore, no special consideration is given to
operation in adverse environments or durability over normal operating conditions in a
research environment.
C.2 Operating Conditions and Specifications
In addition to the originally proposed design, two modifications were made to the
system. First, a support for the driven arm was implemented from 5/8” square aluminum
stock. This 15” support rests under the driven arm to reduce the deflection of the steel
arm. Second, an idler arm offset was added to the idler arm linkage base to provide more
range and reduce the catastrophic effects of the possible mechanical interference. (i.e. the
system will slip rather than seize the motor or break the coupler). This support simply
moves the linkage attachment point to the first quadrant counter-clockwise of the idler
arm linkage base mount. These additional components are shown in Figure C.1.
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Figure C.1 – Driven arm support and idler arm offset components made as modifications to the
original design.
The assembled system has an antenna mount and antenna weight limitation of 10
pounds. This specification must be adhered to in order to achieve the specified life and
performance of the equipment. While overloading may not result in failure, it could
significantly reduce the life of the equipment [16].
To operate the positioning system with the Labview software, the positioning
system must be in the top-dead-center at home condition at the start of initialization. This
position is characterized with the linear track carriage in its “home position” and the
linkage arm 27500 motor steps CW from its “home position”.
It is suggested that in the native configuration presented here, certain parameters
should not be exceeded; these parameters and their values are summarized in Table C.1.
Parameter PDX Command Max Value Set Command
Linear Track Velocity V1 10 1V10
Linkage Arm Velocity V2 10 2V10
Linear Track Acceleration A1 3 1A3
Linkage Arm Acceleration A2 0.25 2A0.25
Linear Track Homing Max 1GH+ 7 1GH+7
Linkage Arm Homing Max 2GH+ 2 2GH+2
Linkage Arm Movement CW
from home position 2D (H+) 2000 steps 2D2000
Linkage Arm Movement CCW
from home position 2D (H-) 75000 steps 2D75000
Linkage Arm top-dead-center (TDC)
from home position 2D 27500 steps 2D27500
Table C.1 – Suggested maximum values for positioning system in native configuration. See [15] for a
complete definition of commands.
Values above those specified in Table C.1 can result in abrupt stops inducing
excessive force on the mechanism and possibly cause the receive antenna to wobble.
Other damage may also occur due to mechanical interference or mechanical limits being
reached. While it is not recommended under any circumstances, if these values are
exceeded, all precautions should be taken to minimize any component flexing or abrupt
stops.
The supporting hardware is all American Standard ¼”, 20 threads per inch
stainless steel screws with corresponding nuts and stop nuts, except where noted. The
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interfacing hardware is metric (the linear and rotary tables are specified metric) 6 mm cap
screws. All hardware is commercially available from local suppliers and spare parts are
located in the MPRG lab. The sealed ball-bearings in the linkage arms are 5/8” O.D.
with ¼” I.D. accepting ¼” hardware. These specialized bearings are available from
McMaster-Carr (part number 60355 K73 – www.mcmaster.com).
Figures C.2 through C.5 illustrate the complete component specifications for the
linkage base (parts 1 and 2), linkage arms, and antenna mount linkage. Given dimensions
are in inches and are design dimensions; manufacturing tolerance may cause variations
on the order of 100 m.
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C.3 Assembly and Removal
To assemble the system, first move the linear table and the rotary table to their
home positions as shown in Figure C.7. Disconnect the power to both motors before
proceeding.
Figure C.7 – Linear and rotary table in home position prior to system installation
Next, remove the two cap screws holding the rotary table to the carriage which are closest
to the linear table drive. Using the blue M6 cap screws, attach the idler arm base linkage
mount to the rotary table base, as shown in Figure C.8.
Figure C.8 – Rotary table with idler arm base linkage mounted to rotary table base
179
Next, attach the driven arm base linkage mount to the rotary table using the two provided
M6 19mm cap screws as shown in Figure C.9. Ensure that the bottom of the mount is
flush with the rotary table base.
Figure C.9 - Rotary table with driven arm base linkage mounted
If using the modified configuration (required for operation with developed software)
attach the idler arm offset to the idler arm base linkage mount using a 1-1/2” ¼-20 screw
and stop nut, otherwise, skip to the next step. Position the idler arm offset so that it is
approximately parallel to the driven arm base linkage mount as shown in Figure C.10.
Figure C.10 – Idler arm offset mounted to idler arm linkage base
The final step is to attach the linkage arm/antenna mount mechanism to the linkage bases
as shown in Figure C.10. To do this, first place driven arm support on top of the driven
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arm mount and affix the driven arm linkage using two 1-1/2” ¼-20 screws while resting
the idler arm on the idler arm offset. Loosely tighten the two screws so there is no
mechanical deflection. Second, using a ¼ inch slim-line open end wrench affix and
tighten the stop nut to attach the idler arm to the idler arm offset as shown in Figure C.11.
At this point, the system will support itself.
Figure C.11 – Attaching the linkage arms to the rotary table via the base linkage mounts.
Next, adjust the position of the idler arm offset so that the two linkage arms are exactly
parallel as shown in Figure C.12. A rigid guide should be used to ensure the bars are
parallel along their entire length. When the bars are parallel, the driven arm base and the
idler arm offset will NOT be parallel. If the linkage arms are not parallel, the relative
position of the antenna cannot be maintained. After making the bars parallel, tighten
down the screw holding the idler arm offset to the idler arm linkage base mount. Figure
C.12 shows the final configuration of the assembled 4-bar parallel linkage. After the
assembly each screw and stop nut should be treated with a machine serviceable adhesive,
such as Loctite© to fix their position. The system is now ready to accept a number of
antenna mounts for positioning operations.
181
Figure C.12 – Assembled 4-bar parallel linkage antenna positioning system.
To attach the PVC antenna mount used in this research, attach the PVC pipe and
antenna to the antenna mounting linkage using 4, #6 machine screws with nuts. Attach
the PVC so that the coax cable extending from the antenna leaves from the hole in the
base of the PVC mount and points away from the mechanism to reduce any interference.
Figure c.13 illustrates proper mounting of the PVC mast.
Figure C.13 – PVC antenna mount attached to antenna mount linkage
182
To remove the system from the Parker Automation equipment, follow these steps
in reverse. Take care when removing the linkage arm/antenna mount mechanism so that
no additional force is place on the idler arm offset or rotary table. Excessive loading
could cause permanent damage to the positioning equipment.
In general, one should not move the positioning equipment with an antenna
affixed to the boom. The arm is not designed to withstand all forces possible through
accelerating or decelerating the entire system with a load attached. When moving the
system with an antenna attached, ensure that movement is fluid and no abrupt stops are
made, to protect both the positioning equipment as well as the antenna.
C.4 Maintenance
To ensure continued proper operation, it is necessary to maintain the positioning
system. First, periodically check all mechanical connections to ensure they are tight and
have not become lose. Due to vibrations and equipment movement, connections not
treated with machine serviceable adhesive or stop nuts are prone to come lose.
Inherent in the design is the possibility for mechanical interference between the
idler arm linkage offset and driven arm linkage. If an interference condition is
encountered follow these steps to safely correct it. First, immediately remove power to
the stepper motor. Second, manually rotate the shaft in the direction to move the arm
away from the interference. Inspect the region where the interference occurred to see if
the idler arm linkage offset or linkage arm show signs of collision. If there is evidence of
collision, inspect the coupling between the steeper motor and rotary table drive. If it is
damaged or broken, remove and replace with a new coupling.
It is necessary to periodically check the RS-232 interfaces on the fan-out box as
well as the index command and position sensor lines (located on the PDX indexer units).
If the wires on the command lines become lose it may cause the track or parallel linkage
to oscillate in a random fashion, as if jammed. If this behavior is observed, ensure that all
of the command wires are securely fashioned in the connector and that the jumpered
wires are still connected. For details on the proper wiring configuration, refer to [15] as
well as the troubleshooting guide.
The ball-screw in both the track and the rotary table periodically need lubrication.
See [16] and [17] for the proper type of lubrication and schedule for this maintenance.
C.5 Troubleshooting Guide
This section presents several common problems encountered during operation of
the positioning system. A list of the problems followed by possible causes and solutions
are presented.
1. Neither the track nor the parallel linkage responds to commands sent. First,
verify that the communication link between the indexer and motor is operating
properly. This can be checked by toggling the first DIN switch on the indexer
labeled “self test”. If the motor moves, the link between the indexer and motor is
OK (see [15] for more information on self test conditions). Second, verify that
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the RS-232 connection is connected to the laptop as well as the fan out box.
Verify that the “track” position sensor and command line are connected to the
“track” inputs of the fan-out box and PDX indexer, respectively. Also, verify that
the “spin” position sensor and command line are connected to the “spin” inputs of
the fan-out box and PDX indexer, respectively. On the fan-out box, verify that
the switches are set to “track enable” and “spin enable”, respectively. Finally,
verify that there are no broken or lose connections between the indexers and
positioning equipment. Make sure that the track is not set against one of its limits
if trying to execute a move command.
2. The track or parallel linkage shakes/oscillates violently when a command is
sent. This problem is most likely due to a loose or disconnected wire on the PDX
indexer connector (black connector that plugs into indexers). Carefully remove
the black connector and verify that all wires are securely in the plug and that
jumpered wires are connected. For details on the proper wiring configuration
refer to [15].
3. The track or parallel linkage will not report status or movement stops after a
homing routine. This behavior is most likely due to a buffer problem with the
RS-232 link. First, physically disconnect the serial connection on the laptop and
reestablish the link. Verify the two way link is operational by sending an R
command. If both indexers are operational the return value should be *R. This is
a good way to check on the status of the indexers. For more information on using
this command, see the programming reference [15].
4. Execution of the Labview application halts after initializing the track and the
track stops moving. This behavior is caused by the motor_done_moving VI (see
Section C.7 for software related issues) becoming stuck waiting for the indexer to
respond with *R, indicating the end of a move. This can be caused by executing
the initialization routine after an abrupt termination of the link or a buffer overrun.
To correct this problem, refer to item number 3. When using a polling technique
to wait on moves, it is imperative that a two way link be established and verified.
5. After apparent normal operation for several measurements the track stops
operating. The serial buffer has a set limit (see [15]) of the number of characters
that can be stored without clearing. This behavior will only occur for a long set of
consecutive instructions or numerous back to back measurements. If this occurs,
terminate the current session; disconnect the serial connection, and then begin a
new session after reconnecting the serial cable. Refer to item numbers 3 and 4 for
similar problems of this type.
C.6 Positioning System Suggested Upgrades
At the time of writing, there are several improvements that can be made to the
existing positioning system to further improve its effectiveness. Hopefully, as time goes
on and further contributions to this system are made, the list will become obsolete.
1. Upgrade the 1/4” plate steel linkage arms to 5/8” square aluminum stock.
This upgrade will reduce the overall weight and reduce the deflection due to the
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antenna mount. Furthermore, it will help eliminate the wobble encountered when
moving the antenna at a high rate of speed.
2. Design and Implement a biasing scheme to eliminate transition regions. This
upgrade will increase the useable repeatable range from approximately 170
degrees to 330 degrees. This will also make the maximum possible coverage area
realizable.
3. Design and Implement a counter-weight to increase the end load capability.
By implementing a counter weight system, the effective moment seen at the base
can be reduced and a corresponding increase in length of the linkage arms or
increase in end load. This system must be implemented while maintaining the
150 lbs maximum weight specification. For details on counter-weighing and
moment arm calculations, see [19].
4. Design and Implement smoother casters for easy mobility. The current
configuration uses removable wood mounted casters which do not turn and bind
easily. A system that allows smooth motion would aid in moving the track.
5. Fabricate linkage arms of various lengths for covering various areas. Larger
or smaller areas (with improved resolution) can be obtained if families of linkage
arms are manufactured. It is imperative however, that the maximum loading of
the system is not violated.
C.7 APAC System Requirements and Additional Support
This section provides additional information on the Antenna Positioning and
Acquisition Control (APAC) application designed in conjunction with the antenna
positioning system. Covered in this section are the required software packages and
drivers as well as details of the algorithm implementations. The APAC VI is available
from MPRG which contains additional information in the form of comments concerning
very specific implementation issues. Furthermore, the APAC CD (on file with MPRG)
contains a directory template and installation files for all supporting programs (not
Labview) for use with the sliding correlator measurement system.
C.7.1 System Requirements
In order for the APAC VI to operate, several additional Labview modules must be
installed, which are all available for download from the internet. The following list
details the requirements, including additional external hardware.
1. PC running Windows 98 or later with one available serial port
2. National Instruments Labview 6.0 or higher (Labview 7.0 recommended) with
Measurement and Automation option installed
3. NI-VISA 2.5 or higher run-time environment for Windows 98/2000/ME/XP
4. TDS 5000 Series Digital Phosphor Oscilloscope Instrument Driver (available
from www.ni.com) or equivalent corresponding to Oscilloscope used
5. NI-GPIB card (or equivalent) and installed drivers
In addition to the requirements listed above, APAC expects a fixed directory
structure consistent with legacy MPRG propagation measurement storage conventions.
185
A sample directory structure is contained with the source files for APAC and repeated
here for completeness.
The VI library APAC.llb should be place in a directory in which the installed
instrument drivers are located (usually the default Labview directory). If the library file
is placed elsewhere, it may be necessary to manually link the drivers to the library the
first time it is opened. The following is a suggested directory structure for use with
APAC. The subfolder structure of Measurements is required for proper operation.
Table C.2 – Directory structure for proper operation of APAC
In this structure, the APAC.llb file is placed in the Labview 7.0 folder. In
configuring APAC the measurement directory field contained in CONFIGURE ALL
should be set to the folder Measurements shown here. The folder
DeleteAfterMeasCampaign must be created manually and the contents of it deleted
regularly. As an artifact of the software, if there are multiple tracks per location,
temporary folders are written to DeleteAfterMeasCampaign to avoid system errors. The
temporary folders will have random names, denoted here by XXX, all of these should be
deleted at the end of a measurement campaign. The folder loc999 must also be created
manually, and by convention is the calibration directory. Within this folder, subfolders
corresponding to the 3 digit transmitter chip rate in MHz must be created (denoted here
by ZZZ). These subfolders are used to store the calibration waveforms and log files.
When a log file is created using CREATE LOG TRACK LOCATION the
location field specifies AAA and the track number specifies BBB. There can be multiple
tracks per location, except they must be written sequentially (an error will occur if
track002 is created and track001 does not exist). The contents of trackBBB will be N2
text files and one log file, pertaining to a grid measurement. There can be an arbitrary
number of locations as long as each has a unique name.
Additional information on the legacy storage structure of propagation
measurements at MPRG can be found in the appendix of [5].
C.7.2 Converting User Parameters to 2-D Grid Definition
As mentioned in Chapter 4, the convention which uses measurements per
wavelength to define the grid adds an additional point to the grid when the number of
measurements per wavelength is less than 1. Figure C.14 illustrates the spacing
186
convention and shows why the additional point is added. The example of Figure C.14 is
one row of a measurement grid which is specified as a two wavelength grid with 4
measurements per wavelength. The top row of numbers corresponds to grid point while
the bottom row corresponds to measurement number of the current wavelength. Since
the convention was arbitrarily defined as shown, to measure a grid which is actually two
wavelengths long, the additional point (denoted by X) must be added.
Figure C.14 – Grid spacing convention used to derive measurement spacing from measurements per
wavelength.
C.7.3 System Specific Parameters
As described in Chapter 4, there are several system specific parameters that will
only change if the native configuration of the system changes. The lower level system
parameters, such as linkage arm length, home reference and motor resolution can all be
accessed by opening the sub VI sub_configure_track. After opening the VI and scrolling
down, the data fields shown in Figure C.15 are accessible. The boom arm length (linkage
length) and home reference are equal and are given by the center to center distance
between the pivot point of the linkage base and the antenna mount. If the lengths of the
linkage arms are changed, these parameters must be changed. The maximum grid length
is determined empirically from the number of motor steps from the positioning system
home to the point of mechanical interference. Similarly, the minimum XY resolution is
calculated using equation (4.4). This should be entered as the worst case linear and
angular resolution. This portion of the VI also allows the user to see the number of motor
steps corresponding to the moves stored in the three positioning vectors [i], d[i], and
sa[i]; i = 0:1:N-1.
(0) (1)
1 2 3 4 1 2 3 4 X
(2) (3) (4) (5) (6) (7) (8)
187
Figure C.15 – Configuration options that can only be accessed through opening the
sub_configure_track VI separately and scrolling down. In the native configuration, these parameters
will never change.
C.7.4 A Note on Modifying APAC for Fast Acquisition
There may be instances where rapid measurements are desired for continuous
motion of the positioning system, for instance in the case of Doppler shift. In its native
configuration APAC does not support this type of measurement. To modify the
application an additional module would be required which significantly reduced the
overhead associated with acquiring waveforms. The two areas this overhead can be
reduced are in the scope acquisition time and APAC file storage time. The scope can be
configured for fast frame acquisition using the existing scope drivers in APAC (refer to
online help for more information). Reducing the file storage time should be addressed by
storing the waveform in the form of two parameters (time start and offset) and values
(voltage) for later reconstruction offline. Incorporating these ideas into a virtual
instrument will be essential in successfully performing fast acquisition.
C.7.5 APAC Suggested Upgrades
At the time of writing there are several suggested upgrades o the APAC system.
In light of these upgrades, it follows what the current limitations of the system are. The
interested researcher is encouraged to address these issues in a second-generation version
of this application.
1. Integrated DSO card operating in the Labview Environment. This
improvement would significantly ease the burden (time and computational) of
acquiring measurements. It would also make it easier for expansion of the
acquisition functionality (such as in fast frame acquires)
2. Control signal generators and PN generators using APAC. This would allow
easier set-up and variation of measurement parameters.
3. Automated calibration process. Making use of initial attenuation, attenuation
step and, number of steps, a VI which semi-automated the process could be
188
implemented. A further improvement would be to make use of digitally
controlled attenuators on the measurement system front end to completely
automate the process.
4. Arbitrary two dimensional measurement grid. The extension to a rectangular
grid would immediately provide more coverage area since the track is 1.2 m long.
Further development could extend to arbitrary grid shapes, such as circular
shapes.
5. Arbitrary positioning anywhere within the measurement grid. The current
configuration allows for only complete sweeps of the grid. Adding a so called
“jog” mode which allowed the user to position the system anywhere within the
grid would be a valuable addition. This feature would allow missed points to be
easily accessed.
6. Implement a “PAUSE” and “EMERGENCY STOP” feature. A pause
feature would allow the measurement to cease if channel conditions suddenly
changed (e.g. a bystander walks in front of the receiver). An emergency stop
would reduce the risk of equipment damage if a possible interference condition is
seen.
7. File writing overhaul. In the current configuration the directory structure for
correct operation is very specific. A possible upgrade would be a routine which
created the directory structure if it did not exist. Furthermore, the need for the
temporary directory DeleteAfterMeasCampaign should be eliminated in any
upgrades.
C.8 Additional Support
In addition to this user’s guide there is information available in the MPRG lab.
This information includes the data sheets for the existing equipment as well as hardcopies
of the design documents and the APAC code. For other support the following references
are helpful:
1. Parker Automation: Daedal Division – www.daedalpositioning.com – linear
table, rotary table, and indexer support.
2. McMaster-Carr – www.mcmaster.com – specialty hardware and materials for
modification needs.
3. National Instruments – www.ni.com – Labview developer and support site
4. Labview Developers Zone -
=labviewzone – code sharing and forum support
5. Labview Instrument Driver Network -
- Specific hardware drivers for
oscilloscopes and other equipment.
189
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Vita
Daniel James Hibbard was born in Williamsburg, Virginia and was raised in Toano,
Virginia; graduating from Lafayette High School in 1998. Hibbard enrolled in Virginia
Polytechnic Institute and State University in the fall of 1998 to pursue a Bachelor of
Science degree in Electrical Engineer. In 2000, he was awarded the Rappaport wireless
communication award for interest in the area of wireless communications.
While at Virginia Tech, Hibbard participated in the Co-Op work experience as an
electrical designer for Mathew J. Thompson III Consulting Engineers in Newport News,
Virginia. As an undergraduate, he was a member of the Tau Beta Pi National
Engineering Honor Society and IEEE, also earning the Engineer in Training (EIT)
designation in 2002. Hibbard graduated Suma Cum Laude in the spring of 2002.
In the fall of 2002, Hibbard began work towards a Master of Science degree in Electrical
Engineering with Virginia Tech’s Mobile and Portable Radio Research Group. Also in
2002, Hibbard was awarded the Harry Lynde Bradley Fellowship for Graduate Study,
which provided full research funding for the duration of his Masters research. In 2003
Hibbard worked as a summer intern at Raytheon in Falls Church, Virginia. He completed
his Masters degree in the spring of 2004 and accepted a full time position with Raytheon
in Falls Church.
Hibbard’s research interests include radio wave propagation, propagation prediction, and
propagation measurement systems as well as spread spectrum communication systems.
Hibbard actively writes and records musical arrangements. He also actively participates
in surfing, snowboarding, and mountain biking in his free time.
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