Using a scope with the same power supply on a different motherboard produced a much more solid value for the CLK signal. No hard drive or graphics activity was represented in the waveform.
I've been probing around a bit on the resistor networks (most reading "B 330J") on the problem board. Each of the ones I have hit have a single white square marked on the PCB to one side - so they should be bussed. That being the case, how much can I really determine from an ohm check with them still in circuit?
Walking one probe across pins 2-8 with the other probe on the common pin while each resistor network is in circuit yields the following (three RN examples) -
Name | pin 2 | pin 3 | pin 4 | pin 5 | pin 6 | pin 7 | pin 8 |
RN1 - | 33 | 650k | 650k | 650k | 650k | 650k | 650k |
RN2 - | 33 | 650k | 650k | 650k | 650k | 650k | 650k |
RN3 - | 33 | 650k | 650k | 2M | 2M | 2M | 2M |
Those that measure 2M on RN3 start near 1.8M and climb quickly with the probe attached. Moving to the next pin in the same RN starts at the same value as the previous pin.
RN3 is far from the previously corroded area.
In a similar fashion, pins B20, B28, and B30 on any given ISA connector on the problem board start at about 1.5M and quickly sail upward when being given a continuity check to ground (ground pin B1 on the ISA slot, specifically). In contrast - B20, the clock pin, held at 4.7k when measured on the working 486 motherboard. Naturally the boards didn't have the exact same values for a matched given pair of pins (i.e. Problem A1 vs Working A1) between them, but a stable 4.7k on working board's B20 vs a sailing 1.5M on the problem board's B20 seems to be a stark contrast.
Pardon my naivete, but can I draw any conclusions from this?