I did a few more experiments with my BC-221 and think that I may
have possibly made the BC-221 better than it was at least before I
started messing with it. That is, of course after it had sat
around for about 80 years. 80 years is a bit hard to comprehend,
but they are that old! By making a few mechanical adjustments I
have brought this particular BC-221 back into top notch
calibration.
I found that very slight movements of the VFO shield plate on the
bottom of the chassis can be used to adjust the inherent
inductance of the coil and bring it back close to the original
settings in your CAL book. There are four screws that hold the
aluminum plate to the unit. I put a pair of 0.030" spacers on the
front two screws located under the chassis. It moved the crystal
checkpoints closer to the original points on the scale. I then
played with the spacing on the back side where the screws go thru
the top of the chassis and secure the shield plate with two
standoffs on the opposite side underneath. This is a BC-221N made
by Philco. Some other units may not have the same shield. All of
these added spacers help to move the aluminum shield a bit farther
away from the ceramic coil. This affects the residual inductance
of the oscillator coil. I tried 0.020 spacers on the rear and saw
the 4.000 MHz checkpoint go above the original value by about 4 or
5 divisions. The original error was +12.4 divisions. So I
increased the spacers to 0.040 and the crystal checkpoint at 4 MHz
was within about -1.6 divisions of where it was back in 1942. That
is awfully close.
My method of testing involved calibrating the BC221 at 2.000 MHz
on the high range and then noting each frequency marker without
touching the corrector knob. My thinking was that the crystal
markers would be close to the "book" value if the coil was exactly
the same as it was in 1942. What I saw was a gradually increasing
error as I moved up from 2.000 MHz. At 4.000 MHz I was 12.4
divisions off what was listed in the book. I then looked at
fixing that error.
Here is a listing of a few iterations across the 2 to 4 MHz
range I compared crystal cal points from 1942, and then 2024
without modifications. Then I show two examples of varying the
coil shield plate by .020" and .040". I also show the cumulative
error from the original 1942 book settings. The dial markings ate
peculiar to only my BC-221, but all of them will show the same
trend I am sure.
2.000 |
0158.8 |
0158.8 +0.0 |
0158.8+0.0 |
0158 +0.0 |
2.1666 |
0566.9 |
568.0 +1.1 |
0567.9 +1.0 |
0567.7+1.0 |
2.250 |
0769.0 |
0770.3+1.3 |
0769.9+0.9 |
0769.8+0.8 |
2.3333 |
0970.1 |
0971.5+1.4 |
0970.6+0.5 |
0970.6+0.5 |
2.500 |
1369.2 |
1371.6+2.4 |
1370.1+0.9 |
1370.1+0.9 |
2.6666 |
1761.8 |
1765.2+3.4 |
1763.8+1.3 |
1762.9+1.1 |
2.750 |
1956.1 |
1959.8+3.7 |
1957.1+1.0 |
1956.9+0.8 |
3.000 |
2525.3 |
2530.2+4.9 |
2526.1+0.8 |
2525.9+0.6 |
3.250 |
3082.9 |
3088.2+5.3 |
3082.8+0.1 |
3082.6-0.3 |
3.3333 |
3266.1 |
3272.8+6.7 |
3266.1+0.0 |
3266.0-0.1 |
3.500 |
3630.0 |
3638.2+8.2 |
3630.1+0.1 |
3629.9-0.1 |
3.6666 |
3988.2 |
3998.1+9.9 |
3989.0+0.8 |
3988.9+0.7 |
3.750 |
4167.3 |
4178.0+10.7 |
4167.8+0.5 |
4167.6+0.3 |
4.000 |
4699.6 |
4712.0+12.4 |
4697.0-2.6 |
4698.0-1.6 |