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Impact of Measurement Errors on the ClosedLoop Power Control for CDMA Systems
Li-Chun Wang and Chih-Wen Chang
National Chiao Tung University, Taiwan
Email : [email protected]
AbstractIn this paper we present a simple analytical modelto evaluate the impact of measurement errors on the closed-loop power control for code division multiple access (CDMA)systems. By introducing a new performance measurement, theprobability of false command in power control, PFC, a closedform formula for calculating PFC with consideration of mea-surement errors is presented. Furthermore, we drive a bit er-ror rate (BER) performance bound in terms of PFC for theCDMA system with the closed-loop power control (CLPC). Theproposed analytical approach can quantitatively evaluate theperformance of the CLPC taking into account of the effects ofmeasurement errors and Doppler frequency under a Rayleighfading channel. Through simulation and analysis, we show thatthe proposed analytical BER bound can accurately estimate theBER performance of the CLPC under the impact of measure-ment errors. Interestingly, we find that the CLPC is less sensi-tive to measurement errors due to the non-linear operation inthe one step up/down power control scheme compared with thevariable-step size power control.
Index TermsCDMA System, Power Control, MeasurementError.
I. INTRODUCTION
AC curate power control is one of key technologies to
achieve high capacity code division multiple access
(CDMA) systems. Power control errors may be resulted
from many factors [1], such as loop delay [2], quantiza-
tion errors [3], multi-path fading [4], [5], link-quality mea-
surement errors [6], and feedback errors [7]. Although the
closed-loop power control (CLPC) in the CDMA system has
been studied extensively in the literature [3], [6], [8], [9],
[10], fewer papers have analyzed the performance of power
control scheme subject to signal-to-interference ratio (SIR)
measurement errors.Previous works about the impact of measurement errors
on power control can be summarized as follows. The im-
pact of measurement errors on the open-loop power control
was studied in [6]. The authors in [1] discussed the filter-
ing effect in the measurement scheme for the WCDMA sys-
This work was supported jointly by the Lee and MIT center for network-ing research, and the National Science Council R.O.C under the contract90-2213-E-009-068, 89-E-FA06-2-4, and EX-91-E-FA06-4-4.
tems. In [10], [11], [12], the issue of joint minimization of
SIR measurement errors and power control errors are inves-
tigated in the form of a stochastic control problem, but the
SIR measurement errors in [10], [11], [12] are modeled as
white Gausssian noise. However, in [13], it has been found
that measurement errors tend to be log-normal distributed incellular channel with Rayleigh fading and shadowing.
The goal of this paper is to develop a simple and accurate
analytical model to evaluate the impact of log-normal dis-
tributed SIR measurement errors on the CLPC of CDMA
systems. The contributions of this work can be summa-
rized in two folds. First, to evaluate the impact of measure-
ment errors on the closed-loop power control, we introduce
a new performance measurement called the probability of
false power control command, PFC. The motivation of in-troducing the new parameter, PFC, is because the feedbackpower control command is the key to the accuracy of power
control scheme. We will present a close-form formula for
calculating PFC in terms of measurement errors. Second,we propose a simple BER bound in terms of PFC. Hence,by using the proposed analytical approach, the performance
for different SIR measurement schemes on the closed-loop
power control in the CDMA system can be easily obtained.
The rest of this paper is organized as follows. In Section
II, we briefly introduce power control and define the proba-
bility PFC. Section III derives the closed-form formula ofPFC in terms of measurement errors. In Section IV, we de-rive a simple BER bound for the CLPC in CDMA systems
with the parameter PFC. Section V shows some analyti-cal and simulation results. Section VI gives concluding re-
marks.
I I . PROBABILITY OF FALSE POWER CONTROL
COMMAND
A. Background
Generally speaking, we can categorize power control
models into two kinds. The first one is the open-loop power
control and the other one is the closed-loop power control. In
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the former scheme, a mobile terminal decides its own trans-
mission power by comparing the desired received SIR and
the target SIR to compensate path loss and shadowing. On
the other hand, the CLPC makes the base station determine
the up/down power control command by comparing the re-
ceived SIR with the target SIR. The block diagram of theCLPC scheme is shown in Fig.1. As shown in this figure,
the CLPC has two feedback loops where the inner loop is
for fast power adjustment, while the outer loop is for setting
the target Eb/No.
B. Probability of False Power Control Command
Because the accuracy of power control commands will
strongly influence the performance of the closed loop power
control, it is important to investigate the impact of measure-
ment errors on the false power control command. Figure 2
illustrates how measurement errors will influence the power
control command. For example, as shown in Fig. 2, if theactual SIR value is below the target SIR value, the CLPC
will issue a power up command to increase the transmis-
sion power. For a small measurement error, the power con-
trol command will still be correct since the measured SIR is
below the the target SIR as shown in the left hand side of the
figure. However, if a large measurement error causes the re-
ceived SIR to become larger than the target SIR, then power
control command may change to be a wrong power down
command, as shown in the right hand side of the figure.
In order to evaluate the effect of measurement errors on
the closed-loop power control scheme, we define the proba-
bility of false command (PFC) in power control as follows.
PFC = Prob{ sgn (SI RT SI RM)= sgn (SI RT SI RA)} (1)
where sgn(x) is the operator to choose the sign ofx, SI RMis the measured SIR, SI RA is the actual SIR value, and theSI RT is the target SIR. From this definition, one can seethat the measurement error makes the sign of (1) change,
thereby issuing a false command in power control.
III. ANALYSIS
In this section, we will derive an analytical formula toevaluate the probability of false command in power control.
To begin with, we model the power control error (PCE) and
measurement errors as independent log-normal distributed
random variable as [9], [13]. Denote the SIR measurement
error by a random variable, Y, and the power control error by
a random variable, X. In the following, we will consider all
the variables in the dB domain. Denote SI RT and SI RA asthe target SIR and the actual SIR, respectively. Then SI RA
Received
Signal
ChannelMatch
Filter
Rake
Combiner
Channel
Decoder
CRC
Detection
Eb/NoMeasurement
Power Control
Step Size
Target Eb/No
Setting
+
T
Fig. 1. The block diagram of the closed-loop power control scheme.
can be expressed as the summation ofSI RT and power con-trol error, X, i.e.
SI RA = SI RT + X . (2)
The measured SIR, denoted as SI RM, can be expressed asthe summation ofSI RA and the measurement error, Y, i.e,
SI RM = SI RA + Y . (3)
From (2) and (3), we know
SI RM = SI RT + X+ Y . (4)
Substituting (2) and (4) into (1), we find that a false power
control command occurs when the following condition is
sustained:
sgn(SI RT (SI RT + X+ Y)) =sgn(SI RT (SI RT + X)) (5)
or
sgn(X+ Y) = sgn(X) . (6)Hence, the probability of false power control command
(PFC) can be written as
PFC = P(X+ Y < 0|X > 0)P(X > 0) +P(X+ Y > 0|X < 0)P(X < 0)
= P(X+ Y < 0, X > 0) +
P(X+ Y > 0, X < 0) . (7)
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Measurement
error Actual Eb/No
Target Eb/No
Measured Eb/No
No False Command
Actual Eb/No
Target Eb/No
Measured Eb/No
However, actual Eb/No < Target
Eb/No. We need to increase power.
Measured Eb/No < Target Eb/No
=>Issue a Power up command
Measured Eb/No > Target Eb/No
=> Issue a Power down command
PCEMeasurement error PCE
False Command occurs.
Fig. 2. Occurrence of false command in power control.
Note that in the dB domain both X and Y are Gaussian ran-dom variables with zero means and standard deviations of
X and Y , respectively. Because
P(X+ Y < 0, X > 0) = P(X+ Y > 0, X < 0), (8)
we can simplify PFC as
PFC = 2P(X+ Y < 0, X > 0)
= 2P(Y < X,X > 0)
= 2
0
x
fXY (x, y)dydx , (9)
where fXY(x, y) is the joint probability density function ofrandom variables Xand Y. Because measurement errors aremajorly influenced by the measurement scheme rather than
power control method, we assume the measurement error Xis independent of power control error Y. Then, we have
PFC = 20
x
12XY
exp(x2
22X)
exp(y2
22Y)dydx
= 2
0
x
1
2XYexp(
x222X
)
exp(y2
22Y)dydx . (10)
Let x
= x/X and y
= y/Y . Then we can express PFCas
PFC = 2
0
X
Yx
1
2exp(
12
x2)
exp(12
y
2)dy
dx
. (11)
Next, we change the coordinate axis to polar coordinate axis
by letting x
= r cos and y
= r sin . Then PFC can bewritten as
PFC = 2
/2tan1
X
Y
0
1
2e1
2r2rdrd
=1
2 tan
1 XY
. (12)
Now we want to analyze the impact of PFC on the BERperformance. From [14], we know that for the received bit
energy to noise density ratio b, the bit error rate of BPSKmodulated signals in Rayleigh fading channel is
Pb1 =1
2
1
b
1 + b
. (13)
In the AWGN channel, the BER of BPSK modulated signals
is
Pb2 = Q(
2b) (14)
where
Q(x) =1
2x
e
t2
2 dx . (15)
Since the purpose of power control is aimed to remove
Rayleigh fading, we expect that the BER performance of the
CLPC will be closed to (14) if the power control perfectly
removes the impact of Ralyeigh fading; and on the other
hand, the BER performance of the CLPC will be close to
(13) if there is no power control. Consequently, we propose
an upper bound on the BER performance for the closed-loop
power control subject to measurement errors as follows.
Pb,FC 2PFCPb1 + (1 2PFC)Pb2
PFC1 b1 + b+(1 2PFC)Q(
2b) , (16)
where Pb1 and Pb2 are defined in (13) and (14). Note thatbecause the maximum of PFC is 0.5, we use 2PFC to ap-proximate the case without power control. We will evaluate
the accuracy of the proposed upper bound (16) via simula-
tion in the next section.
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TABLE I
SIMULATION PARAMETERS.
Spreading Factor 4
Doppler Frequency 5-30Hz
Power Control Period 0.667mSec
Power Control Step Size 1 dBTarget Eb/No 5 dB
Modulation Scheme BPSK
30 20 10 0 10 20 30 400
0.02
0.04
0.06
0.08
0.1
0.12
PCE in dB ( The measurement error is modeled by Log N(0,52) )
Pro
bility
PCE (Simulation)LogNormal Fitting
Theoretical PFC
=0.301
Simulative PFC
=0.309
Fig. 3. The power control error statistics with a measurement error ofstandard deviation equal to 5 dB, i.e. Y =5 dB, with fd = 20 Hz, andtarget Eb/No = 5 dB.
IV. NUMERICAL RESULTS
In this section, we simulate the uplink performance for a
single user under a flat Rayleigh fading channel. We assume
the measurement errors are log-normal distributed random
variables [13]. Other parameters used in the simulation are
listed in Table I.
Through simulation, Figure 3 shows the probability den-
sity function of power control errors (PCE) subject to mea-
surement errors with standard deviation of 5 dB. As shown
in the figure, the PCE (expressed in dB domain) exhibits
the similar characteristics of normal distribution. This re-
sult confirms our assumption that the PCE is lognormal dis-
tributed random variable even with the influence of measure-
ment errors.Figure 4 shows the impact of measurement errors for dif-
ferent Doppler frequencies on the the probability of false
power control command, PFC. One can note that thehigher the Doppler frequency, the lower the PFC. This phe-nomenon can be explained as follows. Because the radio
channel will change faster at a higher Doppler frequency, the
power control mechanism usually cannot follow fast chan-
nel variations. Thus, in this situation a larger power con-
1 2 3 4 5 6 7 8 9 100.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45
0.5
Y
(STD. of measurement error in dB)
PFC
fd=5 Hz
fd=15 Hz
fd=30 Hz
Theory
Simulation
Fig. 4. The probability of false power control command ,PFC, subject tomeasurement errors for different Doppler frequencies, where fd = 30, 15,and 5 Hz, and target Eb/No = 5 dB.
trol error will occur. Due to a larger gap between the tar-
get SIR and the actual SIR, it is less likely to change the
power control command from power up to power down
or vice versa. In other words, a larger PCE due to higher
Doppler frequency can tolerate large measurement errors,
thereby having a smaller PFC as shown in the figure. In Fig-ure 4, we also verify the accuracy of the analytical results of
PFC derived from (12) by comparing with simulation. Asshown, simulation results ofPFC are close to the analyticalresults derived from (12).
Figure 5 shows the corresponding BER performance of
Fig. 4 including the impact ofPFC. Although in Fig. 4 itis demonstrated that a higher Doppler frequency leads to asmaller PFC, the BER performance at a higher Doppler fre-quency is still larger than that at a lower Doppler frequency
as shown in Fig. 5. It is implied that even with a larger
probability of false power control command, the closed-loop
power control scheme under a slower fading channel still
performs better than that under a fast fading channel.
Figure 6 shows the impact of very large measurement er-
rors on the probability of false command PFC in the closed-loop power control. One can see that as a measurement error
increases up to 30 dB, the probability of false power control
command tends to be saturated at 0.45. Note that in (16), the
maximum ofPFC approaches to 0.5 for the infinite measure-ment error.
Figure 7 illustrates the BER performance of the closed-
loop power control subject to very large measurement errors.
As shown in the figure, the theoretical values according to
formula (16) provide a reasonable bound on the BER per-
formance of the closed-loop power control subject to mea-
surement errors. Because PFC will be bounded to be 0.5even with large measurement errors, one can find that the
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1 2 3 4 5 6 7 8 9 1010
3
102
101
Y
(STD. of measurement error in dB)
BER
fd=5Hzfd=15Hzfd=30Hz
Fig. 5. The BER performance comparison of the the closed-loop powercontrol subject to measurement errors for different Doppler frequencies,where fd = 30, 15, and 5 Hz, and target Eb/No = 5 dB.
BER of the up-down closed-loop power control will also be
bounded under a large measurement error. In the figure, with
the target Eb/No equal to 10 dB, the BER is limited to below0.02 even with a measurement error with standard deviation
of 30 dB. Thus, it is implied that the up/down power control
scheme is robust to measurement errors.
Figure 8 compares the up/down closed-loop power con-
trol with the variable-step size closed-loop power control
from the standpoint of the sensitivity of power control er-
rors with respect to measurement errors. In our simula-
tion, the variable-step size power control is a power con-
trol mechanism with higher resolution in power adaptationsteps. As shown, unlike the variable-step power control has
a strong correlation between measurement errors and power
control errors, the impact of a larger measurement error on
the up/down closed-loop power control is less sensitive.
V. CONCLUSIONS
In this paper we have presented a simple and accurate
analytical expression for the probability of false command
(PFC) in the closed-loop power control (CLPC) subject tomeasurement errors. Moreover, we also propose a BER per-
formance bound in terms ofPFC. It is found that the larger
the Doppler frequency, the smaller the PFC, while for theBER performance, a larger Doppler frequency results in a
poor BER performance even with a smaller PFC. Interest-ingly, we find that compared with the variable-step power
control, the up/down CLPC is more robust to measurement
errors due to the non-linear operation in the up/down power
control scheme. The proposed analytical approach can be
easily applied to analyze the performance of the closed-loop
power control with different SIR measurement schemes.
0 5 10 15 20 25 300
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45
Y
(STD. of Measurement error in dB)
PFC
SimulationTheory
Fig. 6. Probability of false power control command, PFC, with a largestandard deviation of measurement error, Y, fd = 30 Hz, and targetEb/No = 5 dB.
5 10 15 20 25 30
103
102
101
Y
(STD. of measurement error in dB)
BER
Target Eb/N
0=5 dB
Target Eb/N
0=10 dB
Upper bound
Simulation
Fig. 7. BER performance of the closed-loop power control against mea-surement errors with stand-deviation,Y, and fd = 30 Hz.
Thus, an interesting future research extended from this work
is to apply the proposed analytical framework to incorporate
different SIR measurement schemes to evaluate the perfor-
mance of the closed-loop power control in CDMA systems.
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