1. Technical Field
The present invention relates to broadcasting RF signals and, more particularly, to improvements in high level combining of analog FM and digital signals.
2. Description of the Prior Art
It has been known in the radio broadcasting art to transmit a composite signal consisting of a frequency modulated (FM) analog signal and a digital signal, such as an in band on channel (IBOC) digital signal. The prior art includes, for example, the U.S. patents to Murphy et al. U.S. Pat. No. 5,315,583 and Papadopoulos et al. U.S. Pat. No. 6,144,705.
The prior art also includes separate amplification of such signals, sometimes referred to as IBOC high-level combining. An example is illustrated in
Because the outputs ν1 and ν2 are combined only after they have reached a high level of amplitude (because they have already been amplified by separate amplifiers) this is referred to in the art as “high-level combining” or “separate amplification”. This type of combining results in high losses. This may be viewed as the penalty paid for the simplicity involved. In a 10 dB coupler, the problems that are noted include the following: the main FM transmitter needs to have enough headroom in order to increase its output power by 11% to overcome the combiner insertion loss. This can be very problematic in specific installations without additional headroom to spare. Major hardware upgrade could be necessary to overcome this issue, such as by replacing the existing main FM transmitter with a more powerful transmitter. A second problem with this type of system is that the overall dissipation increases. Besides the power dissipated by digital transmitter 12, additional energy is wasted at this reject load RL where up to 10% of the main transmitter FM output and up to 90% of the output of the digital transmitter will be dissipated. This inefficiency creates additional heat load for the air-conditioning equipment in the room containing the transmitter equipment.
The present invention is directed toward improvements in the combining of an output of an FM transmitter with that of a digital transmitter. The improvements are directed toward minimizing the FM and digital power losses in high level combining. The improved system provides various benefits including higher overall system efficiency and elimination of requirements for FM headroom.
In accordance with one aspect of the present invention, an apparatus is provided for broadcasting an RF signal comprised of analog FM and digital signals. The apparatus includes a splitter that splits an FM signal received from an analog FM source into a fractional portion and a remainder portion. The summer combines the fractional portion with a digital signal obtained from a digital source to provide a first combined signal. The main FM transmitter amplifies the remainder portion to provide an amplified FM signal and a digital transmitter amplifies the first combined signal to provide an amplified combined signal. A combiner then combines the amplified FM signal with the amplified combined signal to provide a composite RF signal to be broadcast.
In accordance with another aspect of the present invention, a method is provided for broadcasting an RF signal that is comprised of analog FM and digital signals. The method includes the steps of extracting a fractional portion of an FM signal provided by an analog FM source and providing a remainder portion. The summer combines the fractional portion with a digital signal obtained from a digital source to provide a first combined signal. The remainder portion and the first combined signal are respectively amplified by a main FM transmitter and a digital transmitter. The amplified FM signal and the amplified combined signal are then combined to provide a composite RF signal to be broadcast.
The foregoing and other features of the present invention will become apparent to one skilled in the art for which the present invention relates upon consideration of the following description of the invention with reference to the accompanying drawings, wherein:
Reference is now made to
In the embodiment of
It has been determined that the new and improved embodiment in
This system as shown in
Combining Analysis
The combining analysis hereinafter involves significant equations and their explanation with respect to various graphical terms. It is believed that various definitions of terms and language employed should be defined to facilitate an understanding herein. Table 1, presented below, provides these definitions.
When two signals are combined, the instantaneous output voltage ν1(t) is given by the sum of each coupled input voltage:
ν1(t)S12ν2(t)+S13ν3(t)
The average output power, P1, is obtained by averaging, over time, the square of the resultant output voltage:
In the case of coherent signals, the numerator can be simplified as the square of the sum of their rms voltages:
Where ν1, ν2, and ν3 are the corresponding rms values (vectors) for the waveforms ν1 (t), ν2 (t) and ν3 (t).
However, for incoherent signals, as those at different frequencies (FM and IBOC), the total power is obtained by the sum of each coupled power. This can be proven by solving the square of the resultant instantaneous voltage.
S122 ν2(t)2+2S12S13ν2(t)ν3(t)+S132ν3(t)2
Due to orthogonality between ν2 (t) and ν3 (t), their multiplication averages over time to zero, amounting to no contribution to the average power at the output. The resulting term, to be averaged over time, has been reduced to:
S122ν2(t)2+S132ν3(t)2
which means that the average power at the output, for non-coherent signals, is obtained by summing each coupled input power,
P1=S122P2+S132P3
Important to note that this value is smaller than the value obtained by the square of the sum of their rms voltages (properly phased), and accordingly, some power is being lost.
In the following sections, the advantages are noted of adding some coherence between the signals ν2 and ν3, such that the mid term does not totally cancel.
How Much Dual FM Injection is Needed
Partial coherence is obtained by adding some FM signal at port 3, along with IBOC. Let's now determine the minimum amount of dual FM injection that is needed so that the main FM power can remain unchanged.
Assume that ν1 is the output voltage, ν2 is the FM voltage applied at the thru port (where the main FM transmitter connects), and ν3
To further simplify the analysis, make Zo=1, and the total coupled FM power into port 1 (output)=1. Then at 100% TPO, P1=1 and ν1=1:
P1=(S12ν2+S13ν3
Solving for ν3 —fm, the FM voltage needed at the coupled port 3 to achieve output power P1=1:
This expression is used for the condition of no impact on the main FM power. This condition forces ν2=1, and then the value ν3
If we now sweep a range of coupling factors, then we obtain the dual FM injection level that is needed, as a function of the coupler used, in order to make the main FM path lossless.
Table 2, DFM level needed not to impact the main FM transmitter output.
How Much IBOC Injection is Needed
The peak IBOC voltage needed at the coupled port 3 (v3
where κν is the IBOC voltage peak-to-average ratio, in linear terms, needed to comply with the RF mask. A value of 1.778 (5 dB) will be considered throughout the analysis.
The ratio between the IBOC and FM through the digital transmitter is:
Using the case in which the main Tx remains at 100% TPO (ν2=1), and considering a 6 dB coupler, the IBOC/FM ratio needed is −2.5 dBc.
So far it is seen that the required amount of dual FM injection at port 3 increases with the coupling factor, but in general it is a small fraction of the main FM service (or TPO).
On the other hand, the required generation of IBOC at port 3 is inversely proportional with the coupling coefficient. The smaller the coupling coefficient (the looser the coupling) the more IBOC power will need to be generated.
Considering both effects at once, tighter coupling coefficients require more DFM injection but less IBOC generation. The optimum coupling value that minimizes the size of the digital transmitter is now considered.
Optimum Coupling Coefficient for Minimum Size of Digital Transmitter
The peak voltage at port 3 is:
ν3
which generates a peak power of:
This value includes fast, highly compressed envelope peaks. It is the short duration of these peaks, much shorter than the amplifier thermal constant (its temperature will hardly change with modulation) that allows the device to reach higher levels than in a CW mode. Accordingly, in order to compare the size of a digital transmitter, whose envelope is being pulsed, to the corresponding 100% TPO (that is provided by a CW-operated FM transmitter), we need to adjust these peak levels to its equivalent maximum CW operation.
Based on peak power measurements, we rate the maximum CW operation of a digital transmitter 0.5 dB below its maximum pulsed level. As an example, a 11.22 kW peak-capable digital transmitter will be considered to be a 10kW CW unit (10kW=11.22 kW−0.5 dB). This is the value that will be used to compare sizes between the FM and Digital transmitters.
The relative size of the digital transmitter, respect 100% TPO, can then be estimated by:
If we sweep a range of coupling coefficients, and graph three different values of ν2 (main FM output), we then obtain the results as seen in
Several important conclusions can be extracted from
The digital transmitter needs to be 35% the size of the main transmitter's (or TPO), in order to provide the secondary FM injection level that is required to make the main FM-path lossless. It is important to note that this value (35%) is comparable to the size demanded for separate amplification. In other words, with the same hardware (as the one used in prior art), we are now providing a “lossless” solution for the FM path, resolving the headroom problem.
Finally, by using now this tighter coupling coefficient (6 dB), the amount of IBOC that needs to be generated drops by 4 dB, of which 25% will get coupled to the output. As a result, the dissipated IBOC power into the reject load is about 30% of the amount dissipated in separate amplification. The next section studies the reject power in more detail.
Optimum Coupling Coefficient for Minimum Reject Power
The total reject power is composed of:
Preject=Preject
where,
Preject
and,
To keep our analysis practical, let's select the same size transmitter as the one required for separate amplification (minimum size).
With this restriction, the total FM voltage supplied at port 3 will be limited to:
As the coupling coefficient is changed (or swept), and the digital transmitter size is now allowed to change, we will have to adjust the output of the main FM transmitter (ν2) in order to guarantee 100% TPO at the output of the combiner (ν1=1)5.
The value of the voltage at port 2 then needs to be:
The minima in total reject power is found to be somewhere between 6 to 7 dB coupling, with a value equal to half of the power dissipated in separate amplification.
Output Power of a Digital Transmitter Operating with DFM
Considering signal clipping to be our limit (independent of their probability of occurrence), let's calculate the maximum average power at which a digital transmitter can be operated, for different IBOC injection levels.
P3=P3
Substituting, we obtain:
The total output power of the digital transmitter, relative to its CW equivalent rating, has been plotted in
The new operating average power, with a DFM injection of −2.5 dBc, is about the same than the IBOC-only rating.
We can already predict an improvement in the overall system efficiency, i.e., with the same generated average power of the digital transmitter (respect separate amplification), we have upgraded our system to FM IBOC without demanding 11% more power out of the main FM transmitter.
Efficiency of a Digital Transmitter Operating with DFM
The measured efficiency of a digital transmitter, operating at different levels of DFM injection is represented in
For IBOC/FM ratios weaker than −10 dBc, the efficiency of a digital transmitter is very similar to the efficiency of common amplification. For stronger injection levels, the efficiency quickly improves (for the same average power) and approaches the efficiency of IBOC-only operation.
Overall System Efficiency
Knowing that the output power (including IBOC) has to be 1.01, the overall system efficiency is:
We will assume a 60% efficiency for the FM transmitter η2. The efficiency curve fit function used to generate the graph in
A graph of the overall efficiency for a DFM system implemented using the minimum size digital transmitter, is represented in
With the new DFM implementation, the efficiency approaches 50%, as compared to separate amplification, whose efficiency would be 46%. The coupling coefficient for peak efficiency is found at 6.75 dB.
We have described the Dual FM injection, an improved high-level combining method of upgrading to IBOC. This method uses a tighter coupling coefficient at the output combiner, which decreases the IBOC losses. Simultaneously, by injecting a small fraction of the FM signal, properly phased, at the coupled port, the total combining efficiency is increased, as both the main and the dual FM injection are partially summed at the output.
A coupling factor of 6 dB is the optimum value to minimize the size required for the digital transmitter and to reduce the dissipation in the reject load, and as such boosting the overall system efficiency by 3 to 4%. Under these conditions, the total reject power is expected to be reduced by 50%.
All these benefits are added to the fact that with DFM injection, the main FM transmitter does not have to increase its output level to overcome the coupler losses, an inconvenience at times unsurpassable for many installations in the field.
Finally, the system performance is dependent on the size of the digital transmitter in the following manner; the bigger the digital transmitter to be used, the stronger the FM injection through it and the tighter the optimum coupling coefficient can be, this way obtaining a lower output power demanded of the main FM transmitter, a lower reject power and a higher overall system efficiency.
It has been determined that this system of high-level combining with dual FM injection achieves lower insertion loss for the FM transmitter. Instead of a 10% insertion loss known in the prior art, the typical insertion loss for the new system is 0 dB (no loss), if a 6 dB coupler is used. If tighter couplers are used, an actual gain is achieved, as more FM power is added through port 2. This improvement is fundamental to economically upgrade to IBOC in “difficult powers” where the FM insertion loss can not be tolerated if prior art is to be used. Overall efficiency of this new system can be as high as 52% using present broadcast technology, which results in a reduction of 20% in dissipated power. The RF combining efficiency can reach 98.5% with typical values of 95%. The equipment ratio to make the conversion is now 1.35. The small difference of 4% in size (minimum), in practice is enough to provide optimum configuration to broadcast customers.
Although the invention has been described in conjunction with a preferred embodiment, it is to be appreciated that various modifications may be made without departing from the spirit and scope of the invention as defined by the appended claims.
Number | Name | Date | Kind |
---|---|---|---|
4507746 | Fletcher, Jr. | Mar 1985 | A |
4660192 | Pomatto, Sr. | Apr 1987 | A |
5029003 | Jonnalagadda | Jul 1991 | A |
5315583 | Murphy et al. | May 1994 | A |
5436930 | Bremer et al. | Jul 1995 | A |
5465396 | Hunsinger et al. | Nov 1995 | A |
5757854 | Hunsinger et al. | May 1998 | A |
5838799 | Cioffi et al. | Nov 1998 | A |
5859876 | Dapper et al. | Jan 1999 | A |
5949793 | Bossard et al. | Sep 1999 | A |
5991334 | Papadopoulos et al. | Nov 1999 | A |
6014407 | Hunsinger et al. | Jan 2000 | A |
6144705 | Papadopoulos et al. | Nov 2000 | A |
6166774 | Plonka | Dec 2000 | A |
6487256 | Kroeger et al. | Nov 2002 | B2 |
6563880 | Hunsinger et al. | May 2003 | B1 |
6721337 | Kroeger et al. | Apr 2004 | B1 |
6898249 | Kroeger et al. | May 2005 | B2 |
6914579 | Schadler | Jul 2005 | B2 |
6982948 | Kroeger et al. | Jan 2006 | B2 |
7088740 | Schmidt | Aug 2006 | B1 |
7170950 | Wildhagen et al. | Jan 2007 | B2 |
20040048586 | Monson | Mar 2004 | A1 |
Number | Date | Country | |
---|---|---|---|
20050190851 A1 | Sep 2005 | US |