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* NOTE: The following ASCII text file (without graphics) *
* is contained in a printed technical paper available *
* from Broadcast Electronics Inc. Unfortunately, it *
* was not possible to reproduce the graphics portions *
* of this paper within this text file. If you find the *
* information in this file of interest, you may request *
* a complimentary, printed, copy including figures and *
* graphics from: BROADCAST ELECTRONICS INC. *
* P.O. BOX 3606 *
* 4100 N. 24TH STREET *
* QUINCY, IL. 62305-3606 *
* ATTN: SALES DEPARTMENT *
* PH 217-224-9600 *
* FAX 217-224-9607 *
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* The contents of this technical paper are *
* Copyrighted (c) 1983, by Broadcast Electronics Inc. *
* All rights reserved. *
*********************************************************************
TRANSMITTER PERFORMANCE REQUIREMENTS
FOR SUBCARRIER OPERATION
John T.M. Lyles - Mukunda B. Shrestha
Broadcast Electronics, Inc.
Quincy, Illinois
I. INTRODUCTION.
Stereophonic subcarrier operation has made FM broadcasting the profitable
radio medium of today. SCA subcarriers, on the other hand, have not attained
the same level of acceptance, partly because of crosstalk with the main pro-
gramming channels, and partly because of the desire to maintain maximum modula-
tion levels. The key to optimal subcarrier performance requires examination of
the entire transmitting system and subsequent correction of the bandwidth and
distortion limitations of all stages through the chain. This approach was used
during the development of a new line of FM transmitters. Specific design im-
provements in FM exciter linearity, stereo and SCA generator spectral purity,
and amplifier bandwidth and stability have allowed new levels of performance
with simplified field adjustments.
Subcarriers commonly use either AM-on-FM modulation (as in stereo) or FM-
on-FM modulation (as in traditional SCAs). Both processes are complicated by
the principle that frequency modulation requires transmission of an infinite
number of sidebands for perfect demodulation of information. In practice, how-
ever, the information on FM can be carried in a broadcast channel with accep-
tably low distortion. There are two different frequency bands involved:
(1) The composite baseband, which contains the modulating audio plus one or
more amplitude or frequency modulated subcarriers, and (2) the FM carrier
frequency band of the transmitter.
Waveform linearity, amplitude bandwidth, and phase linearity must be main-
tained at acceptable limits in the baseband chain from the audio inputs through
subcarrier generators to the FM exciter modulated oscillator. From here, the FM
carrier is usually amplified in a series of class C nonlinear power amplifiers,
where most amplitude variation is removed. However, the amplitude and phase
responses of all the networks which follow must also be controlled to minimize
degradation of the subcarriers.
Figure 1b shows the effects of a narrowband RF bandpass filter on the RF
spectrum of a composite signal consisting of a stereophonic subcarrier modulated
only on the left channel with 4.5 kHz and with a 67 kHz unmodulated SCA sub-
carrier. The only distortion evident on the spectrogram is the loss of some
sidebands greater than 150 kHz from the center frequency and amplitude differ-
ences between the lower and upper sideband pairs. Figure 1d shows the corre-
sponding effects observed on the demodulated baseband spectrum for the same
signal. Note the creation of many undesired intermodulation terms which could
cause crosstalk into both the stereophonic and SCA subcarrier bands.
FIGURE 1a. FIGURE 1b.
WIDEBAND RF SPECTRUM TO DEMODULATOR BANDWIDTH LIMITED RF SPECTRUM TO
DEMODULATOR
FIGURE 1c. FIGURE 1d.
DEMODULATED BASEBAND SPECTRUM FOR DEMODULATED BASEBAND SPECTRUM FOR
WIDEBAND RF SPECTRUM BANDWIDTH LIMITED RF SPECTRUM
SHOWING DISTORTION PRODUCTS
II. ELEMENTS OF FM BROADCASTING SYSTEM WHICH AFFECT SUBCARRIERS.
The following components affect subcarrier performance through the system:
1. SCA generator
2. Stereo generator
3. FM exciter
4. Composite STL, when used
5. All transmitter RF amplifiers
6. Antenna system, including diplexers and combiners
7. Multipath and other propagation phenomena
8. Receiver antenna, IF passband, and demodulators
This paper will concentrate on components which are part of the transmit-
ting equipment. Information pertaining to receivers, multipath, antennas, and
combiner effects can be found in other articles and reports listed at the end of
this paper.
2.1 SCA Generator.
The SCA generator frequency modulates a subcarrier with band-limited audio
information or data. Audio frequency shift keying and direct FSK for data chan-
nels can be used with some new generators. Multiple narrowband or a single
wideband SCA can be used in the baseband. The audio frequency response of the
standard narrowband SCA must be tailored to prevent the FM sidebands of the SCA
from overlapping the stereophonic sidebands by greater than -60 dB. With a 67
kHz SCA, to minimize crosstalk from the SCA into the stereophonic subchannel,
the audio should be bandlimited to 4.3 kHz and the peak deviation of the sub-
carrier limited to 6 kHz or less. Various Bessel function tabulations have been
prepared for use with 67 kHz FM SCAs, and can be found in the NAB handbook.
Any system utilizing new center frequencies, multiple subcarriers, or different
modulation forms will require careful spectral analysis of the baseband to
assure minimum interference and maximum compatibility with stereo.
The SCA generator should produce a subcarrier sinewave with low harmonic
distortion, requiring minimal bandpass filtering as bandpass filtering of FM can
generate additional unwanted intermodulation products in the demodulated SCA
information. The audio input should be preconditioned by a filter, as mentioned
above.
A modern high-performance SCA generator, shown simplified in Figure 2, uses
a linear VCO IC. It produces a sinewave at any frequency from 39 to 95 kHz with
less than 0.5 percent distortion. A 100 kHz low-pass filter is used on the
output. The audio input is conditioned with a 6th order low-pass filter which
is 3 dB down at 4.3 kHz. This filter may be bypassed for wider bandwidth SCAs
or different preemphasis. A dc coupled data input is included for direct
frequency shift keying. Note that the subcarrier output is faded on and off at
a controlled decay rate rather than switched to prevent squelch noise with the
SCA receiver.
FIGURE 2. SIMPLIFIED BLOCK DIAGRAM OF FC-30 SCA GENERATOR
2.2 Stereo Generator.
The stereo generator must have good 38 kHz subcarrier suppression with mod-
ulation applied. Excessive 38 kHz leakage may cause additional 76 kHz regenera-
tion in the system. The stereo generator must also have good 76 kHz (second
harmonic) suppression. The second harmonic modulation sidebands should be at-
tenuated as well, because they add crosstalk into the SCA subchannel. For an
SCA signal to noise ratio of -60 dB the stereophonic harmonics should be sup-
pressed by -70 dB. This number allows for some degradation through the entire
system. Manufacturers of stereo generators have traditionally chosen either
linear or switching modulators.
The linear modulators may use balanced analog circuits with adjustable 38
and 76 kHz null controls. These adjustments should be maintained if excessive
76 kHz becomes evident using spectrum analysis of the baseband. The switching
modulator is popular because of less critically toleranced components and good
longterm stability. However, the modulator waveform usually requires filtering
with a steep cutoff 53 kHz low-pass filter. This filter is not a trivial
design, because passband amplitude ripple and phase non-linearities cause
degraded high frequency separation by adversely affecting the upper sideband of
the L-R subcarrier.
The stereo generator shown in Figure 3 uses a digital stairstep generator
to synthesize the subcarrier and pilot simultaneously, eliminating any pilot
phase variation. Appropriate components are added in the synthesis to approx-
imate a sinewave with lower harmonic content. The composite low-pass filter
then has a gradual rolloff, with the -3 dB point beyond 100 kHz. Separation is
better than 50 dB at 15 kHz. In this design, subcarrier suppression is spec-
ified at -75 dB and the 76 kHz sidebands are -80 dB below 100% modulation. At
57 and 95 kHz, the third and fifth pilot harmonics, suppression is -80 dB or
more.
Audio input low-pass filters are necessary in all stereo generators. These
"brickwall" filters protect the pilot and subcarrier by greatly attenuating
audio components above 15 kHz. Some designs have filters which ring or
overshoot on transient program waveforms due to poor passband group delay. This
overshoot can be measured as overmodulation. Without audio low-pass filtering,
increased spectrum occupation and spill over into the SCA band occurs. If the
pilot level is observed fluctuating during modulation, defective filtering may
be suspected. The FS-30 generator uses carefully aligned 5-pole active low-pass
filters with controlled delay equalization to keep overshoot below 2 dB, while
providing adequate protection to the pilot, stereophonic subcarrier, and SCA
subcarrier.
FIGURE 3. SIMPLIFIED BLOCK DIAGRAM OF FS-30 STEREO GENERATOR
2.3 FM Exciter.
The exciter characteristics are foremost in importance for good subcarrier
performance. The frequency modulated oscillator in most current units consists
of a varicap diode VCO. The voltage-to-capacitance transfer function of these
devices is not linear over the wide range used, so linearization may be neces-
sary. Non-linearities in the FM oscillator can, by altering the waveform of the
baseband signal, create distortion in the demodulated output at the receiver.
A secondary effect of this distortion may include stereo crosstalk into SCA.
Modulator linearization using a piecewise approximation pre-distortion network
has reduced harmonic and intermodulation distortion to less than 0.05% in the
FX-30 exciter (Figure 4). All exciter stages after the oscillator operate as
broadband amplifiers with minimal bandwidth limitations.
FIGURE 4. SIMPLIFIED BLOCK DIAGRAM OF LINEARIZED FM MODULATOR
2.4 Composite STL.
The composite STL is really a transmission subsystem within a system. STL
transmitter requirements are identical to those of the FM exciter and power am-
plifiers detailed in this paper. For minimum degradation of the composite sig-
nal it is recommended that all SCA channel information be fed into the exciter
at the transmitter. Telephone company landlines or another narrowband link can
usually handle the program bandwidths of SCAs. This reduces the technical bur-
den of maintaining very low intermodulation performance through the entire STL
modulation/demodulation process. However, the STL should have a flat bandwidth
through 53 kHz for minimum stereophonic subcarrier degradation. For stereo-
phonic separation of 50 dB, it is necessary to maintain a composite amplitude
flatness of 0.04 dB and phase linearity within 0.2 degrees through 53 kHz in
the baseband. Many exciters and STLs cannot meet this requirement. The stereo
generator should be engineered to compensate for this deficiency through the use
of a built-in composite equalizer with low and high frequency adjustments. The
range of amplitude correction of the FS-30 stereo generator is shown in Figures
5a and 5b. These figures show the maximum boost and cut with the low (Figure
5a) and high (Figure 5b) frequency controls at both ends of their ranges.
FIGURE 5a. FIGURE 5b.
RANGE OF FS-30 LOW FREQUENCY EQ RANGE OF FS-30 HIGH FREQUENCY EQ
2.5 RF Power Amplifiers.
The remainder of the FM transmitter consists of a chain of power amplifi-
ers, each having from 6 to 20 dB of power gain. Ideally, the transmitter should
have as wide a bandwidth as practical with a minimum of tuned stages.
Broadband solid-state amplifiers are preferred to eliminate tuned networks in
the RF path. A new generation of class C bipolar and MOSFET broadband
amplifier stages exhibit both high efficiency and greater than 20 percent
bandwidth to cover the FM broadcast band. These solid-state amplifiers may be
combined for higher power. Tuned output band-pass filters may still be
necessary when operated in a dense RF environment to prevent intermodulation
from being generated in the PA modules.
Higher powered transmitters in the multi-kilowatt range may use a single
tube PA stage with high efficiency. The dollars/watt economics of single-tube
transmitters outweigh the bandwidth benefits of solid-state transmitters at the
higher power levels with present technology. Design improvements in tube-type
power amplifiers have concentrated on improving bandwidth, reliability, and cost
effectiveness.
III. POWER AMPLIFIER CIRCUIT DESIGN.
3.1 Bandwidth Considerations.
As mentioned earlier, the FM signal theoretically occupies infinite band-
width. In practice, however, truncation of the insignificant sidebands (typi-
cally less than 1 percent of the carrier) makes the system practical by accep-
ting a certain degree of signal degradation. The input and output tuned cir-
cuits of the PA limit the bandwidth of the FM signal. The degree of bandwidth
reduction is a design constraint which affects the gain and efficiency in all
tuned PA stages.
The bandwidth of an amplifier is determined by the load resistance across
the tuned circuit and the output or input capacitance of the amplifier. For a
single-tuned circuit, the bandwidth is proportional to the ratio of capacitive
reactance to resistance:
BW = _____1____ =_Xc_ (eq. 1)
2 PI f R C R
where BW = bandwidth between half-power points
f = operating frequency
R = load resistance (appearing across tuned circuit)
C = total capacitance of tuned circuit (includes stray capac-
itances and output or input capacitances of the tube)
Xc = capacitive reactance
The load resistance is directly related to the RF voltage swing on the tube
element. For the same power and efficiency, the bandwidth can be increased if
the capacitance is reduced.
3.2 Grounded-Grid Versus Grid-Driven Operation.
Since the input capacitance of tube amplifiers in a grounded-grid config-
uration is smaller than that of a grid-driven configuration by as much as 50
percent, an investigation was carried out in 1982 to determine the advantages of
using a grounded-grid circuit for a tetrode tube amplifier. Input capacitances
of typical tubes are shown in Table 1.
TABLE 1
TUBE TYPE Cin (pF)
Grounded Grounded
Grid Cathode
4CX3000A 67 140
4CX3500A 58.5 111
4CX5000A 53 115
8990/4CX20,000A 83 190
Prototype input circuits were developed for grounded-grid and grid-driven
operation of a 5 kilowatt PA using the Eimac 4CX3500A tetrode. A series of
measurements were made to evaluate the performance of grounded-grid versus
grid-driven operation of the tetrode PA with respect to gain, efficiency, ampli-
tude bandwidth, phase bandwidth, and synchronous AM under equivalent operating
conditions. Measurements were made at normal and reduced plate voltage for both
saturated and unsaturated PA operation. Saturation is noted when little change
in output power occurs with increasing drive power. Maximum efficiency occurs
at this point. The PA gain and efficiencies are tabulated in Table 2. Swept
amplitude and phase responses of the different PA configurations are shown in
Figures 6a thru 6d.
The significant findings of the tests and measurements are as follows:
1. When driving the PA into saturation, the bandwidth of the PA is limited
by the output cavity bandwidth in the grounded-grid amplifier. The PA
bandwidth in the grid-driven amplifier is limited by the input circuit
Q, which is basically determined by the extent of swamping resistance
used. PA bandwidth under saturation can be improved in either config-
uration by reducing the plate voltage as evident from equation (1).
This involves a trade-off in efficiency with a smaller voltage
swing. For example, in the grid-driven saturated configuration a 25
percent bandwidth improvement was observed with 1.4 dB loss of PA gain
and 2.3 percent efficiency loss with reduced plate voltage.
2. When the PA is not driven into saturation, the grounded-grid amplifier
does not appear to give any bandwidth improvement over the grid-driven
amplifier at the 0.25 dB points (see Figures 6c and 6d). At the 3 dB
points however, there is a slight ( 15%) improvement in bandwidth
when using the grounded-grid unsaturated PA.
TABLE 2
MEASUREMENTS FROM 5KW PA IN GRID-DRIVEN(GD) AND GROUNDED-GRID(GG) CONFIGURATION
CONFIGURATION GD GG GD GG GD GG GD GG
PA CONDITION ---- SATURATED ---- ---- UNSATURATED ----
RF POWER OUTPUT (W) 4900 5000 4800 4900 3225 3350 3325 3200
PLATE VOLTAGE (V) 5220 5200 4500 4480 5320 5315 4550 4600
PLATE CURRENT (A) 1.27 1.26 1.49 1.4 0.81 0.9 1.08 1.0
DRIVE POWER (W) 140 280 190 340 70 170 70 175
EFFICIENCY (%) 73.9 72 71.6 72.7 74.8 66.5 67.7 65.8
GAIN (dB) 15.4 12.5 14.0 11.6 16.6 13.0 16.8 12.6
SYNCHRONOUS AM (dB) -54 -56 -56 -58 -46 -48 -51 -52
FIGURE 6. MEASURED AMPLITUDE AND PHASE RESPONSES OF GRID-DRIVEN
AND GROUNDED-GRID TETRODE POWER AMPLIFIERS
3. A grounded-grid saturated PA improves bandwidth over a grid-driven
saturated PA at the expense of amplifier gain. A 15 percent improve-
ment in the PA bandwidth was observed while losing 3 dB of the am-
plifier gain. For a grid-driven amplifier, a 25 percent reduction of
input circuit resistive swamping results in the same 15 percent band-
width improvement at the expense of only 0.5 dB in gain.
4. The phase linearity in the 0.5 dB bandwidth appears to be better using
the grid-driven PA. The grounded-grid PA exhibits a more nonlinear
phase slope within the passband, yet has a wider amplitude bandwidth.
This phenomenon is due to interaction of the input and output circuits
because they are effectively connected in series in the grounded-grid
configuration. The neutralized grid-driven PA provides more isolation
of these networks, so they should behave like independent filters.
In view of the findings listed above (in particular item No. 3), the use of
a tetrode in a grounded-grid configuration did not appear to be economically
feasible. An additional intermediate power amplifier would have been required
to fulfill the higher drive power requirements, thereby affecting the overall
cost and reliability of the transmitter. The decision was made to use a grid-
driven PA for our FM-3.5A and FM-5A transmitters. Bandwidth limitations of the
grid-driven PA were overcome by swamping the input circuit and by developing a
novel impedance-matching device to achieve optimum transfer of power from the
driver stage into the PA. The loss of PA gain due to swamping was limited to
0.5 dB, while achieving bandwidth nearly equivalent to a grounded-grid ampli-
fier, yet providing a more linear phase response.
3.3 Broadband Impedance-Matching.
A broadband impedance matching circuit was developed to match the high grid
input impedance of a tetrode RF power amplifier to the 50 Ohm impedance of a
solid-state driver. The conventional matching circuits used in transmitter
applications are generally of the type known as L, PI, or T networks. All of
these circuits require interactive adjustment of one or more circuit elements to
provide a satisfactory impedance match for each frequency and RF power level.
The new impedance-matching circuit developed for the FM-3.5A and FM-5A
transmitters consists of a combination of series inductor (L) and shunt capac-
itor (C) circuit elements, implemented as a printed circuit with inductors and
capacitors etched into a copper-clad laminate. Multiple LC sections match the
50 Ohm source impedance to the high input impedance of the grid-driven RF power
amplifier. The impedance-matching device is shown in Figures 7 and 8.
This impedance-matching circuit improves transmitter operation and main-
tainability, compared to previous methods. A single tuning control in the input
circuit is sufficient to tune and match the 50 Ohm driver impedance to the high
input impedance of the grid over the 88-108 MHz FM broadcast band with a 4:1
range of RF power levels. The input-matching circuit eliminates separately
mounted components which can be microphonic (sensitive to vibration) due to
mechanical instability. By incorporating this new impedance matching device, we
have been able to improve the bandwidth, reliability and stability of the trans-
mitter.
The typical performance figures of the FM-3.5A and FM-5A transmitters with
regard to PA bandwidth, efficiency, gain, and synchronous AM (measured for 3500W
and 5000W power outputs, respectively) are presented in Table 3.
FIGURE 8. PHOTO OF INPUT MATCHING DEVICE. TUBE SOCKET GRID RING
CONNECTION AT RIGHT OF CENTER, 50 OHM INPUT AT LEFT
TABLE 3
TYPICAL PERFORMANCE OF TRANSMITTER PAs
BE Model 3dB Bandwidth Efficiency Gain Synchronous AM
FM-3.5A 1.2 MHz 75% 14.5 dB -47 dB
FM-5A 1.3 MHz 75% 15.0 dB -51 dB
3.4 Power Amplifier Cavity.
The vacuum-tube power amplifier is constructed in an enclosure containing
distributed tank circuit elements for minimum loss. The efficiency of the PA
depends on the RF plate voltage swing, the plate current conduction angle, and
the cavity efficiency. The cavity efficiency is related to the ratio of loaded
and unloaded Q as follows:
N = 1 - _Q_ x100 (eq. 2)
Qu
where N = efficiency in percent
Q = loaded Q of cavity
Qu = unloaded Q of cavity
Loaded Q depends on the plate load impedance and output circuit capaci-
tance. Unloaded Q depends on the cavity volume and the RF resistivity of the
conductors due to skin effects. A high unloaded Q is desirable, as is a low
loaded Q, for best efficiency. As the Q goes up, the bandwidth decreases. For
a given tube output capacitance and power level, loaded Q decreases with plate
voltage or with increasing plate current. This explains the improved bandwidth
for the reduced high voltage measurements in Table 2 and Figures 6b and 6d.
Other methods popular in improving the bandwidth of PA output circuits in-
clude minimizing added capacitance, as manufacturers of quarter-wave cavities
have attempted. The ideal case would be to resonate the plate capacitance alone
with a "perfect" inductor, but practical quarter-wave cavities require either
the addition of a variable capacitor or a variable inductor using sliding con-
tacts for tuning. An inherent mechanical and electrical compromise in these
designs has always been the requirement for a plate blocking capacitor and the
presence of maximum RF current at the grounded end of the line where the con-
ductor may be nonhomogeneous. A new approach to VHF power amplification uses a
folded half-wave cavity design. This is shown compared to conventional designs
in Figure 9. The half-wave line is tuned without the use of variable capacitors
or sliding contacts. The blocking capacitor is unnecessary and the high
current point is located in the central area of the tank line where no joints,
fasteners, or obstructions occur. This design is inherently more
reliable, and due to the folded nature, requires only slightly more physical
height than the quarter-wave design.
FIGURE 9. COMPARISON OF PA CAVITIES
The bandwidth of the PA cavity is optimized by a choice of the highest
characteristic impedance mechanically allowable. The center conductor is sized
for minimum impedance discontinuity and is directly clamped to the outer surface
of the anode fins for best heat transfer. The secondary tuning line (with ad-
justable bellows) is sized to maintain a similar characteristic impedance with-
out appreciable end-loading distributed capacitance. An inductive loop couples
the strong fundamental magnetic field near the center of the cavity. The loaded
Q of the cavity varies as the square of the effective loop area and inversely
as the square of the distance of the loop center from the cavity center axis.
This loop is positioned so that it links more or less magnetic field and
determines the output loading of the transmitter. This unique approach yielded
the bandwidths in Table 3 which provide excellent subcarrier operation.
3.5 PA Adjustments For Subcarrier Optimization.
The power amplifiers which have been discussed operate with improved reli-
ability and power efficiency without compromising subcarrier performance. By
providing a broadband input matching circuit with a single control, adjustment
of these transmitters for optimal subcarrier performance (minimum crosstalk,
maximum separation, etc.) is very repeatable. A typical adjustment procedure
involves tuning the transmitter for minimum audio output from an envelope de-
tector while FM modulating the transmitter to 100% with a single 400 Hz tone.
When the minimum is reached, the audio output from the envelope detector will
double in frequency to 800 Hz. This indicates correct tuning at the center of
the passband. Tuning for best synchronous AM should simultaneously result in
high efficiency. This also coincides with minimum stereo-to-SCA crosstalk. The
rigid mechanical construction of both the input matching circuit and the folded
half-wave cavity contributes to the overall electrical stability of the tuned
circuits, a benefit for long-term SCA operation where constant "tweaking" is
undesirable.
IV. CONCLUSION.
The development of new FM transmitting equipment requires attention to de-
sign details in bandwidth and linearity of all sub-systems, including the stereo
and SCA generators, the FM exciter, and all RF amplifier stages. New
techniques have been developed which reduce the number of controls throughout
the transmitting system, minimizing field adjustment. The key design criterion
for new transmitters is to optimize SCA and stereophonic subcarrier performance
while retaining high reliability.
ACKNOWLEDGEMENTS.
The authors are grateful to Mr. Geoff Mendenhall for his assistance in
editing this paper. The authors also wish to thank Charlotte Steffen for pre-
paring this manuscript and Mike Hayden along with Jeff Houghton for providing
illustrations.
For Further Information On The Technical Aspects Of Stereo/SCA Operation.
Bott,H., "Analysis of Certain System Characteristics of Stereo and SCA
Operation", IEEE Transactions on Broadcasting, Vol. BC-13, January 1967.
Bartlett,G., ed., NAB Engineering Handbook, National Association of
Broadcasters, 1975.
Clark,G., "Let's Minimize Those FM Transmitter Problems", Broadcast Engi-
neering, February, 1974.
Clark,K., and Hess,D., Communication Circuits: Analysis and Design,
Addison-Wesley Publishing Company, Second Edition, 1978.
Denny,R.,Jr. "Report on SCA Operation", Proceedings of 37th NAB Engineering
Conference, 1983.
Federal Communications Commission Rules and Regulations, Vol. III, Part 73,
Government Printing Office, October, 1982.
Gray,L., and Graham,R., Radio Transmitters, McGraw-Hill Book Company, 1961.
Federal Communications Commission, "FM Subcarriers", Docket 82-536.
Hedlund,L., "Stereo and SCA Are Totally Compatible In FM Broadcasting",
Communications News, April, 1974.
Hidle,J., Priester,H., and Resnick,A., "Modulation Levels During SCA Trans-
mission", Broadcast Engineering, February, 1984.
Kean,J., "The Effect of Additional SCA Subcarriers on FM Stereo Performance
and RF Protection Ratios", Proceedings of 37th NAB Engineering Conference, 1983.
Kean,J., "What is SCA Interference and "Birdies"?", SCA Techtalk from NRBA
bulletin.
Klein,H., "Issues Concerning Modulation Levels During FM SCA Operation",
Proceedings of 37th NAB Engineering Conference, 1983.
Lanier,R., "FM SCA: An Engineering Perspective", Broadcast Management/
Engineering, September, 1983.
Mendenhall,G., "The Composite Signal-Key To Quality FM Broadcasting",
Broadcast Electronics, Inc.
Mendenhall,G., "SCA Basics", Telocator, September/October, 1983.
Middlekamp,L., "Stereophonic Separation in Transmission", IEEE Transactions
on Broadcasting, Vol. BC-14, September, 1968.
Motorola, Inc., "Subsidiary Communications Authorizations, and Their
Application To Radio Paging", Motorola, Inc., Communication Sector Paging
Division, September, 1983.
National Association of Broadcasters, Westinghouse Broadcasting and Cable,
Inc. and National Public Radio, "Increased FM Deviation, Additional Subcarriers
and FM Broadcasting: A Technical Report", Comments on BC Docket No. 82-536,
August 30, 1983.
Onnigan,P., "Transmitting Antenna VSWR Effects on FM Stereo", Jampro
Antenna Company.
Schober,E., "FM Multipath and Distortion Reduction Through RF Amplifier
Optimization", Broadcast Engineering, May, 1983.
Schrock,C., "FM Broadcast Measurements Using the Spectrum Analyzer",
Tektronix Application Note 26AX-3582-3.
Waldee,S., "SCA and Stereo FM", Audio, January, 1979.
Weirather,R., and Hershberger,D., "Amplitude Bandwidth, Phase Bandwidth
Incidental AM, and Saturation Characteristics of Power Tube Cavity Amplifiers
for FM", IEEE Transactions on Broadcasting, Vol. BC-29, March, 1983.
Weirather,R., and Smith,S., "Design Criteria for Multi-station Combining
Systems", Proceedings of 37th NAB Engineering Conference, 1983.