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Authors: Darioush Agahi, William Domino
Conexant Systems Inc.
Newport Beach, CA
Note: This article originally appeared in the
June 2000 edition of "Applied Microwave & Wireless" (now out of print)
Both authors now
work for Skyworks Solutions Inc.In the design of wireless portable devices, antenna efficiency
is a variable that can have a great effect on overall system performance, and yet may not always receive
the attention it deserves. As an example, RF engineers must frequently make critical tradeoffs in receiver
design in order to improve sensitivity by mere fractions of a dB, but a poor antenna efficiency can
easily cause a degradation of several dB. This pitfall can occur in systems such as GSM, where many
tests are performed using a cable connection to the antenna port; a handset may easily pass such tests,
only to be later hampered by its antenna in the field. This paper is targeted at the very important
parameter of antenna efficiency, and a measurement technique that can be used to quantify it.
Antenna “efficiency” must be distinguished from antenna “gain”. Antenna gain is a directional quantity
that refers to the signal strength that can be derived from an antenna relative to a reference dipole.
Efficiency, on the other hand, quantifies the resistive loss of the antenna, in terms of the proportion
of power that is actually radiated versus the power that is first delivered to it. It is not a directional
quantity.
The Model
We model the antenna’s loss as a resistor placed in series with the radiation resistance, as shown
in Figure 1. Since the model includes no reactances, there is an implicit assumption that the measurements
must be taken at resonance. The equations to be derived later require this assumption.
Figure1 Model of Antenna Loss
The antenna efficiency (see appendix) is
h =
(1)
Note that it is immaterial whether the antenna is matched to the source resistance R_{S}.
While it is certainly desirable and necessary to match the antenna in actual use, the match is not part
of the problem of finding the above resistance ratio. Therefore we need only relate the radiated power
to that which is transferred forward at the point shown in Figure 1. What is needed, then, is a way
to effectively separate the resistances R_{LOSS} and R_{RAD} by way of measurement,
so that the efficiency can be calculated.
The Wheeler Cap
Wheeler [1] sets forth just such a method, where a hollow conductive sphere is placed over the antenna
at the radius of transition between the antenna’s energystoring nearfield and its radiating farfield.
This transition radius occurs at a distance of l/2p, and thus the sphere is referred to as the “radiansphere”. The
role of the conductive sphere is to reflect all of the antenna’s radiation while causing minimal disturbance
to the nearfield. In theory, a complete sphere is appropriate for reflecting the radiation of a small
dipole, which is an approximation of an isotropic antenna, while in practice a monopole with a ground
plane can be capped with a halfsphere. The halfspherical “Wheeler cap” is shown in Figure 2. For 900MHz,
the cap’s radius is 5.3cm.
Figure 2 HalfSpherical Wheeler Cap
If all of the power radiated by the antenna is reflected back by the cap and not allowed to escape,
then in our model this is the equivalent of setting R_{RAD} to zero. By making separate S_{11}
measurements with the cap in place and with the cap removed, we gather enough information to find the
resistances and the antenna’s efficiency.
The spherical or halfspherical cap is intended for physically small antennas; simple dipole or monopole
antennas must therefore also be electrically short. Given the cap’s radius, it is not possible to fit
a monopole of length l/4 under it. To test such an antenna
we replace the halfspherical cap with a cylindrical cap, keeping the radius at
l/2p. Such a cylindrical
cap is shown in Figure 3.
Figure 3 Cylindrical Wheeler Cap
Efficiency of Short Antennas: The ConstantPowerLoss
MethodFor an electrically short antenna (< l/10),
the radiation resistance is typically small in comparison to the 50W source resistance of the measuring system. The radiation resistance
of an ideal short monopole [2] is
R_{RAD MONO} =
(2)
So, for example, a 1/20wavelength monopole, which fits comfortably under the halfspherical cap,
exhibits about a 4W radiation resistance. With such a small
value of R_{RAD}, the power lost in the resistance R_{LOSS} is about the same whether
the cap is in place or removed, that is, with zero or finite R_{RAD}. With the assumption of
constant power loss, we can make use of S_{11} magnitude measurements with the cap on and off
as follows:
Cap on. The radiation resistance is zero, and the antenna reflection coefficient
is measured and referred to as S_{11WC. } Then
(3)
Cap off. The radiation resistance is that of the antenna radiating into free space, and the antenna
reflection coefficient is measured and referred to as S_{11FS.} Then
(4)
We need only measure the magnitudes (and not the signs) of S_{11WC} and S_{11FS}.
The antenna efficiency becomes
h =
(5)
h =
(6)
The efficiency can therefore be found directly from the reflection coefficient magnitude measurements,
without any need to actually determine R_{RAD }and R_{LOSS}. It should still be noted
that the measurements must be made at resonance, because the loss model is based on vector S_{11}
values that are allreal, even though only their magnitudes are needed in the above equations.
Eq. (6) appears in [3] in a survey of previous techniques. This method was likely developed to make
it possible to obtain an antenna efficiency measurement using only reflectometertype reflectioncoefficient
measurements, where only the magnitude of S_{11} is measured. In this case the method further
depends on the close proximity of the minimum of S_{11} to its allreal point. For our
example of a 1/20wavelength monopole, suppose the measurements areS_{11WC}
= 0.966
S_{11FS} = 0.823
Then the efficiency calculated from eq. (6) is
h = 79.3%
This antenna causes a performance penalty to the radio of10log(79.3%)
= 1.0 dB
Such an efficiency is not atypical, and some antennas have been measured to be even less than 50%
efficient, which corresponds to a power loss of more than 3dB. This power loss is a direct degradation
of the receiver sensitivity and the transmitter output power, relative to a cableconnection test. Such
a transmitter power loss would greatly degrade the handset’s battery life, and, in cellular systems
that tend to be uplinklimited, it would affect the ability of the handset to obtain service in marginal
areas. In a 1/8dutycycle GSM system operating at full transmit power of 2W with a 50% efficient antenna,
the resistive heating of the antenna would amount to 1/8W!
Efficiency of ModerateLength Antennas: The ConstantLossResistor
Method As the antenna becomes longer, its radiation resistance increases, and the
assumption of constant power loss with and without the cap breaks down. In this case a method of efficiency
measurement that directly makes use of the quantities R_{RAD} and R_{LOSS} is preferred.
Fortunately, modern vector network analyzers can provide a direct display of the impedance of a measured
device when performing a reflection coefficient measurement. So we make use of the resistance ratio
in (1) rather than the power ratio:
h =
(7)
Here the key assumption is that R_{LOSS} itself, rather than the power lost in it, remains
constant with the cap in place or removed. If desired, we can still express the efficiency in terms
of the reflection coefficients: Cap on. The radiation resistance is zero, and the antenna reflection
coefficient is S_{11WC. } Then
(8)
Cap off. The radiation resistance is that of the antenna radiating into free space, and the antenna
reflection coefficient is S_{11FS.} Then
(9)
(7) and (8) are transposed to become
(10)
(11)
And the efficiency is
h =
(12)
h =
(13)
Eq. (13) is actually more accurate then eq. (6) regardless of the absolute value of R_{RAD}
(and thereby of the antenna length). Its one disadvantage lies in the fact that the signs of the (allreal)
S_{11} measurements must be retained and accounted for in the calculation, making for somewhat
less convenience. But it exactly reproduces the resistance ratio at any level of antenna efficiency,
as opposed to eq. (6) which becomes less accurate at lower efficiencies.
As an example, consider
a lowefficiency monopole, where the S_{11} measurements are:S_{11WC}
= 0.626
S_{11FS} = 0.325
Then the efficiency calculated from eq. (13) is
h = 54.9% = 2.6dB
while that calculated from eq. (6) is
h = 32.0% = 4.9dB
The value of efficiency calculated by the constantpowerloss method is unnecessarily pessimistic.
This discrepancy between the methods occurs with longer antennas that inherently exhibit a large R_{RAD}.
Next we plot the calculated efficiency vs. a swept value of R_{LOSS}, in order to further
compare the two methods of calculation. Figure 4 is plotted for an R_{RAD} of 4W (our shortantenna case) while Figure 5 is for an R_{RAD}
of 14W (a longer antenna). In the 4W case the curves agree down to about 75%, while in the 14W case they quickly diverge. In either case the constantlossresistor
method is more accurate, as it agrees with the resistance ratio. This illustrates that the constantpowerloss
method is accurate only for small radiation resistances and high efficiency.
Figure 4 Efficiency vs. R_{LOSS} for Antenna with 4W Radiation Resistance
Figure 5 Efficiency vs. R_{LOSS} for Antenna with 14W Radiation Resistance
Making the Measurements: Practical Considerations
In the above derivations it was assumed that the radiation and loss resistances are not accompanied
by any reactive impedances; therefore the S_{11} measurements need to be made at the antenna’s
actual resonance, as defined by the point where S_{11} is allreal. For an ideal lossless antenna
and perfectlyreflecting Wheeler cap, the S_{11} measurements would be 1 with the cap on and
zero with the cap off, and we need to find the points of allreal impedance that most closely approach
these. They may or may not be precisely the same as where the magnitude S_{11} is minimized,
as illustrated in Figure 6, and so it is advisable to view the measurements on a Smith chart display
rather than a logmagnitude grid. These points should not be too far apart.
Figure 6 Smith Chart Display of FreeSpace S_{11}
It is especially true that the free space measurement should be done at the actual resonance instead
of the antenna’s nominal operating frequency F_{0}. This is because the antenna is normally
loaded down when installed on the handset, and it is expected that there should be a small shift when
it is removed and placed on a different ground plane. A rule of thumb that is normally used for the
maximum limit of this shift is ± 10% of F_{0}. Detuning
beyond this could impact the accuracy of the measurement, as it means the actualusage environment differs
too much from the measuring setup.
Figure 7 Allowable Detuning for Measurement
Conclusion
The Wheeler cap provides a convenient and reasonably accurate method of determining antenna
efficiency. For practical use it consists of a cap over a ground plane, usually of a simpler shape than
the ideal halfsphere, such as a cylinder, keeping the l/2p radius. The efficiency is best determined by measurement of the
antenna resistance with the cap in place and removed, each taken at the resonance defined as the allreal
impedance point.
Appendix
The derivation of equation (1), which also appears in ref. [2] page 48, is duplicated here.
In the ideal case, where there are no disturbances to the antenna, and a perfect match, the input resistance
represents the dissipation loss of the antenna. This resistance represents the sum of radiation resistance
and ohmic resistance.
R_{in} = R _{RAD} + R_{LOSS
}(a1)
_{ } Given that the peak current flowing in to the antenna is I_{in} then
the average power dissipated in an antenna is
Pin = ½ R_{in}  I_{in}
^{2
}(a2)
^{ } Inserting (a1) into (a2) yields,
Pin = ½ ( R _{RAD} +
R_{LOSS})  I_{in} ^{2} = ½ R _{RAD}
 I_{in} ^{2 }+ ½ R_{LOSS}  I_{in}
^{2}
Or equivalently,
P_{RAD} = ½ R _{RAD}
 I_{in} ^{2}
(a3)
P_{LOSS} = ½ R_{LOSS}
 I_{in} ^{2}
(a4)
Using the efficiency equation and inserting (a3) and (a4) yields,
h
=
=
=
After canceling similar terms, it yields,
h
=
References:
1) H. A. Wheeler, “The radiansphere around a small antenna,” Proc. Of the IRE, vol.47,
pp.13251331, Aug. 1959. 2) W. L. Stutzman and G. A. Thiele, Antenna Theory and Design,
Wiley, New York, 1981. 3) R. H. Johnston, L. P. Ager, and J. G. McRory, “A new small antenna
efficiency measurement method,”
IEEE 1996 Antennas and Propagation Society International Symposium, vol.1, pp. 176179
Authors:
Darioush Agahi, P.E. is director of GSM RF systems engineering at Conexant Systems Inc. in
Newport Beach CA. He has 17 years of industry experience of which the last 4 years he has been with
Conexant and 9 years with Motorola’s (GSM) cellular subscriber division. Darioush received his BS in
electronics (1981) and MS in Medical Engineering from the George Washington University in Washington
DC (1983). Also he received an MSEE from Illinois Institute of Technology in Chicago Illinois (1993)
and an MBA from National University in 1997. Darioush holds ten US patents and several more pending,
he is a Professional Engineer (P.E.) registered in the state of Wisconsin. William Domino
is Principal Engineer, GSM RF Systems, at Conexant Systems Inc. in Newport Beach, CA, where he has been
employed since 1992 in the area of digitalradio system architecture development. He received the BSEE
degree from the University of Southern California in 1979 and the Master of Engineering from the California
State Polytechnic University, Pomona, in 1985. His interests currently include receiver and transmitter
system design for various cellular standards, as well as filter design. In these areas he has one patent
issued and ten patents pending.
