Ok I will do this in parts, one, because I don't want to cover each part in a full essay type approach, and put people to sleep, and also allow people to ask questions or add input. I have been following this thread for some time, and I certainly don't want to offend anyone. I think it's great that everyone has given input to the discussion. BUT, I feel it is nessasary to chime in, and add my input to the discussion.
Let's start with the "sandbar" resistors and choke issue....
First of all, while the components MAY eventually increase in resistance, this will affect the idle curent to the transistors. Each board, or set of to transistors has a switched voltage divider supply going through contact of the relay, that are also used to carry the RF output of the amplifier as well. The purpose of the chokes, is to allow both (the DC source present during TX for the bias supply to both boards, and the meter lamp) and the RF output path for the amplifier as well. If the chokes were not there, this arrangement would not work at all. They allow you to share the same relay contacts, traces, and paths for both, the bias, and the RF out while keeping them electronically isolated. That's all there is to it. It also allows you to use the same contacts on the relay.
So, if the components which we have thus far referred to as "sandbar resistors" which are actually called *wirewound resistors" and will be referred to as such for the purpose of this discussion, in this case, change value, which would be really rare, but could happen, the only thing that will happen is that the set of transistors (not both sets, since they each have their own voltage divider supplying bias, respectively) will not have foward bias, it will be lower than normal, or fluctuate. If the small 1.6 or 1.8 ohm (depending on model, week, year, etc) counter part that is the second part of the voltage divider increases in value, or opens (burns out) you would have ay too much current and the transistors would just burn up from too much forward bias. Once again, rare, but I have seen it happen. That is why, with the amplifier keyed, it is important to make sure you have between .48 and .68 volts with the amplifier keyed, with no drive. This will tell you right away if the bias circuit is OK, and all associated components. Depending on temperature of the heatsink (read: transistors) and supply voltage, it will vary, but should be around this range. If it is too low, then the wirewound (sandbar) resistor or resistors have increased in value. If too high, the small 1.6 or 1.8 ohm resistor needs checked, or you have a leaky transistor (2SC2879, 2SC2290, etc) and also, if you have a leaky transistor, the voltage will be there all the time, weather the amp is keyed or not. (remember, in these amplifiers the bias is switched and should only be present during TX mode)
Moving on...
The statement that "harmonics are in the bias supply" is just downright obsurd. I don't want to offend anyone, but it makes no sense, what-so-ever. I will explain. First of all, the 10uf chokes used to keep 27Mhz (28mhz, whatever) off of the bias supply look like a huge amount of resistance at that frequency. So although they allow DC to pass with no issues, at RF it looks like a big resistor. The RF flows to the path of least resistance, so it doesn't get back into the bias supply, at least on paper. To make sure it is "snuffed" out, there are bypass capacitors to ground that take care of what may have gotten past the chokes.
Ok, now that we understand that part... let's dive a bit deeper. While this circuit works well at 27Mhz, let's talk about what a harmonic is. It is a multiple of the fundamental frequency. So, the second harmonic of 27Mhz would be 54Mhz. At this frequency, the chokes and bypass capacitors would be EVEN MORE efficient at removing any RF from the bias path, not to mention what I left out before is that the 25 ohm wirewound resistors (sandbars I cringe saying it that way) also would act as chokes as well at 54Mhz. So that theory is just crazy. Not to mention this this amplifier is a push pull design, and by nature cancels out the second harmonic very well. The third harmonic, same thing, but just better. The ferrite mix, the chokes, bypass caps and resistors all would definetly keep any amount of the third harmonic off the line as well.
The ONLY thing that would effect SWR in, or out, in an arrangement like this, is that if the bias supply changes, it can and will affect the input and output impedance of the transistors a little, which would cause the INPUT SWR to change a bit. It would also detune the output a little as well.
Let's go ahead and stop here, and next time we will go into the input and output circuit and impedance matching curcuits of the amplifier, and I will also go into some simple changes that can be done, especially on the newer DX500 / DX500V designs using the DEI transistors that can be done to bring the input SWR of the amplifier down which will allow your radio to drive the amplifier properly, and not foldback power if it is an HF rig, and if it's not, it will keep your radio cooler, as it will "see" a flat match into the amplifier. This is important too, to help with IMD, or distortion products. No more changing coax length, or other band-aid fixes.
We will also go into some RF bypassing, which will keep RF off of the positive lead, exiting the amplifier, and also the output circuit as well, as how we can better match it to the output impedance of the transistors, and get it to about 52-58 ohms or so over a 3Mhz bandwidth so that we can get more power output, and less heat as well that is wasted in untuned circuits.
But, as I am very busy these days, we will take it one step at a time.