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Before yesterdayVE7SL - Steve - Amateur Radio Blog

Finding Your Best Crystal Radio 'DX Diode'


Over the past few weeks I’ve had time to examine many dozens of diodes, mostly germanium, in my crystal radio diode collection. Many of them were removed from equipment built in the '50s and '60s (old diode matrix boards), some are vintage NIB 1N34As while others are modern SMD Schottky style diodes.

 
There are numerous excellent websites such as this one by Dick Kleijer or  SV3ORA's site  ... all describing elaborate ways to determine which diode is ‘the best one’ (the holy grail diode!) for crystal radio work. Most methods use a vigorous, somewhat complex test procedure plus a lot of math, most of which is well beyond my old brain, in attempts to flesh out each diode’s inherent characteristics ... as the sites referenced above illustrate, the simple appearance of a crystal diode belies its complexity and determining  diode behaviours can be more challenging than one might suspect.

My testing procedures were much more basic, and in the end, may hopefully reveal the best diode in my collection. I think one needs to undertake this with the understanding that there really is no overall ‘best' crystal radio diode but rather, only a diode that is best for your particular system and what works best in my system may not necessarily be the best one in yours.
 
My plan was to measure a few diode behaviors, shrink the list of candidates and then compare them against each other in my system's high-Q tank circuit.
 



My first step was to measure Vf or the forward voltage needed to ‘turn the diode on’. This can usually be determined to reasonable accuracy by using the diode test function on most digital multimeters. I’ve always supposed that the diode with the lowest Vf  turn-on threshold would probably be the most sensitive, but is it the only factor? Hopefully my tests would indicate if anything else is in play.
 
The next task was to determine the minimum signal level of a 1000 Hz modulated carrier on 1400 kHz that could be detected by each candidate diode. An RF probe was used to measure the level of signal capacitively coupled into my crystal radio’s antenna tuning stage which was then lightly coupled  into the detector stage, using the diode under test. No importance was given to the actual base level of this signal other than to note the level at which it could first be detected by ear (using sound powered phones) and making sure the coupling distance between stages remained the same for all diodes under test. This allowed me to compare weak-signal diode ‘sensitivity’ to the diode’s previously measured turn-on point or Vf value. Would the diode with the lowest Vf also be the most sensitive when used in a detector circuit composed of complex impedance, resistance, reactance and capacitance values that the test diode would be looking into?
 
The RF signal coupling was adjusted so the injected carrier could be varied between 0 and 10mV as measured on the RF probe. For each diode, the signal level was slowly increased from ‘0’ until the 1400kHz tone-modulated AM signal could first be detected.
 
The lowest 'first detected' signal level was .6mV while the highest level required 3.4mV, representing a pretty good range of diode behaviours. There were 49 different diodes in the test pool.
 
Four of the 49 diodes detected the .6mV signal, six detected the signal at .7mV, and nine first detected the signal at .8mV. The remainder required a still higher level of injected signal. The average level of first detection was 1.2 mV.
 
Of the four .6mV ‘best detectors’, their turn-on Vf values ranged from .15V to .38V while the .7mV and .8mV detectors had a Vf between .181V and .40V!
 
It seemed, not surprisingly, that generally the higher the Vf turn-on threshold, the greater was the level of signal injection needed for first detection … but evidently using the Vf value alone to determine the ‘best diode’ was not the hard axiom I had always assumed it to be!
 
Since a low Vf was not necessarily needed for good sensitivity, would there by any other tests that might indicate best performance?
 
The next trial was to measure actual diode currents in my hi-Q detector while receiving a lightly-coupled constant level input signal (1400kHz) to see how this value related to Vf. Measured diode currents (Id) varied from 9uA to 14uA for the same level of input signal, with the diode having the lowest Vf also producing the lowest current level ... hhhm! There was more to this than I expected, but generally, the lower valued Vf diodes tended to produce the most current and consequently the louder headphone signal … but not always! Some diodes with a Vf as high as .46V yielded high currents!
 
This now begged the question, “Does the higher current diode with a higher turn on (Vf) prove to be a better overall performer than the diode that turns-on early but produces a weaker signal?” What is the relationship between diode current and weak signal detection?
 
The next step was to express the relationship mathematically by calculating the ratio between the diode’s Vf and the level of diode current  (Id) measured in the previous test (Id / Vf). Each diode could then be assigned a number (Vdx) that might possibly indicate it’s true performance potential in my own system.

The diodes with the highest Vdx values would then be A-B tested under real receive conditions to see if any (or just one!) particular winner(s) might emerge … and if Vf was as critical as initially believed.
 

The Vdx values proved most interesting and seemed to account for some of the anomalies noted in earlier measurements with some of the higher Vdx values coming from diodes not necessarily with a low Vf. I’m hoping that this sorting concept properly takes into account both turn-on level (Vf) and current level (Id), since a higher level in either number will compensate for a lower level in the other. Vdx values ranged from 23 to 66, with seven diodes in the higher 53-66 range.



Click Image For Larger View


All of the 49 diode's test parameters were put onto a spreadsheet and listed in order of their Vdx value.


Click Image For Diode Spreadsheet Data


The highest Vdx assignment of 66 went to my 40-year junkbox resident, a JHS Sylvania 1N3655A microwave mixer diode. It will be interesting to see if it really is the best of the lot! Although it did not produce the loudest signal (Id) compared with others, its Vf turn-on was an impressive .181V and its weak-signal detection level was good although not the lowest. A couple of the UHF diodes exhibited the interesting behaviour of picking up the UHF data stream 'clicks' from my nearby wifi booster. The 1N3655A was one of them.
 
1N3655A Vf = .181V Id = 12uA Vdx = 66
   

Diode #2, with a Vdx of 62, is a mystery diode with a very low Vf of .197V. It was slightly louder and oddly enough, dug down slightly further than the 1N3655A, which had a slightly lower Vf. Although I don’t recall specifically, I suspect the diode may have been removed from a VCR front end many years ago.
 

Mystery diode  Vf =.197V  Id = 12.2uA Vdx = 62
 

Diode #3 with a Vdx of 61 is a modern SMS7630 Schottky microwave detector diode in an SMD package. Although it did not produce a competitive level of loudness (Id) in the diode current test, its shockingly low Vf turn-on of .147V and weak-signal detection threshold were the best of all diodes tested. Before testing, all SMD diodes were mounted on small PC boards in order to attach leads.
 

SMS7630 Schottky  Vf = .147V  Id = 9uA Vdx = 61


Diode #4 (Vdx of 60) is an ISS98, another modern Schottky microwave detector. I recall seeing this diode recommended for good performance in an FM crystal radio detector. Its sensitivity level was excellent.
 

ISS98 Schottky Vf = .211V  Id = 12.5uA Vdx = 60


Diode #5 (also with a Vdx of 60) appears to be a normal germanium of unknown type. I suspect it was used as an RF mixer since it was found on a small printed circuit board with three others, connected in a diode ring configuration typically seen in balanced RF mixers. It produced high current as well as good weak signal capability. 
 

Mystery diode Vf = .22  Id = 13.2uA Vdx = 60


Diode #6 (Vdx of 55) also looks like a germanium of unknown type with a body striping of gray-white-green-gray. If the last band is ignored, this could be a 1N895, a UHF germanium diode. It shows the typical internal cat-whisker type of junction often seen on the 1N34 germaniums.
 

Mystery diode Vf = .238V  Id = 13uA Vdx = 55


Diode #7 with a Vdx of 53 is marked as a ‘95481’ on a green body. It had excellent sensitivity and produced a strong signal (Id), elevating it to the top tier to be looked at more closely.


'95481'  Vf = .246V  Id = 13uA Vdx = 53


Diode #8, another germanium mystery, earned a Vdx of 49 due to its fairly high Id level.



Black 'T'. Vf = .258V  Id = 12.5uA  Vdx = 49


The rather beat-up looking Diode #9 is marked with what appear to be house numbers, '1846' and '6628'. I believe this was pulled from an old portable radio's FM section many years ago. Interestingly, like some of the UHF mixer diodes, '1846 / 6628' detects my high speed modem data stream clicks. Additionally, this tortured specimen produced the highest level of signal among all 49 diodes, with an Id of 14uA.


Vf = .294V  Vdx = 48 Vdx = 14 (Schottky?)


Diode #10 appears to be the brother of Diode #8 with a Vdx of 48. Although it has a lower turn-on point and was a better weak signal detector, it did not produce as much Id as its sibling, dropping it one notch lower on the list. Like its brother, it also has the mystery 'T' marking. Both are most likely unmarked 1N34As.

Vf = .252V  Id = 12 Vdx = 48


As well, three other diodes garnered my interest. Although they ranked lower than I expected, all had previously been found to be good detectors in my system. Their lower ranking may be a hint that my system of grading is not a valid method of determining best performance. All three will be given a harder look in the upcoming elimination tests.

The first is the germanium FO-215. Often touted as 'the holy grail' crystal radio diode but I have never found it to be particularly outstanding. Maybe my system has a lower Q than it really needs in order to show its stuff. This diode is shown on the bar graph above as #11. During testing, it appeared much less capable of weak signal detection than most others but its low Vf and high Id elevated its overall ranking.

Vf = .272V  Id = 13uA  Vdx = 48


The second diode is the Soviet-era D18, a military-grade germanium in a glass '50s-style package. I have previously found it to be a very good detector but its high turn-on level lowered its ranking. The D18 appears on the bar graph as #12.



Vf = .366V  Id = 12.2uA Vdx = 33


The third diode is a vintage Sylvania 1N34 from the 50s and likely one of the first 1N34s to be manufactured. Although it produces a loud signal, its Vf was higher than expected. As I recall, it was salvaged from an old parted-out Heathkit.  It appears on the bar graph as #13.


Vf = .335V  Id = 13uA  Vdx = 39


As mentioned earlier, one can measure and calculate a large amount of data for crystal diodes while they sit passively on the bench but they really need to be mounted, tested and compared in the actual system in which they will be used. Comparing diodes 'A-B' style in real time with weak signals may be better than any measurements made on a diode being bench-tested. 

Will a new ‘holy-grail’ emerge from the pile? This type of testing requires a lot of careful listening so time will tell. 

Testing will be ongoing over the summer / fall months ... stay tuned for the final results, hopefully in time for the fall DX season!

January's Crystal Radio DX Contest

 

The first time I was involved with a crystal radio DX contest was about 20 years ago when I built a well-performing crystal receiver for the Yahoo Crystal Radio Group's annual DX contest. It was a great learning experience and taught me much about circuit losses and how to overcome them. I originally built several sets but was unable to hear anything other than local stations until I eventually figured things out ... the system was only as good as its weakest link or links!


Fast forward to more recently when I obtained and wrote about the Heathkit CR-1 Crystal Radio, a simple but very well-designed tuner that has become popular with collectors. Using the CR-1 re-kindled my interest in the DX contest activity of years ago and when talking with two other amateurs that had an interest as well (one had also been in the earlier contests sponsored by the now defunct Alabama Crystal Radio Group), we decided to bring the contest back once again. The Facebook Crystal Radio DX Contest Group was formed last fall, a set of rules drawn up and the contest date set for the first week of January of this year. This gave interested participants plenty of time to build something they could use in the contest.

I spent all of December designing and constructing a new contest radio, hopefully one with enough selectivity to get around the 15 local flamethrowers (10-50kW S9++ signals) that plague the band for me and eventually drove me from crystal radio activities.

The new radio makes use of several 'traps' to null strong signals ... two are in the antenna line while one is loosely coupled inductively to the detector tank circuit. The two inline trap coils are wound with Litz wire on ferrite toroids (R40C1) while the third is a basket-wound Litz coil (660/46) on a 4" diameter form.


The antenna tuning stage also uses the same ferrite material but in the rod / bar form. I wound a low-end as well as a high-end coil for the tuner using the same high-count Litz as on the big trap coil. The low-end coil is wound on a bundle of three rods while the high-end coil uses a single rod.

Antenna tuner

The detector stage uses another Litz coil with this one being solenoid-wound on a 4" diameter form. Both the antenna tuner and the detector use excellent quality hi-Q ceramic insulated air variable capacitors (18-360 pfd). All components that handle RF are insulated from the plywood bases in order to reduce losses. Moving a capacitor from the plywood to the insulated standoffs makes a noticeable difference, something learned the hard way years ago but actually measured while using the new radio.

Detector stage
 

The detector also has provisions for comparing various diodes as not all diodes are created equal ... not even all diodes with the same number! When testing and comparing diodes of the same type such as the popular 1N34 germanium, every once in awhile one of them will turn out to be noticeably more sensitive than the others. In my built-in B-A-C diode test module, the hottest diode is always mounted in middle-position A, making it easy to quickly compare by switching to the left for B or to the right for C. So far the best one I have found is the vintage Russian D18 germanium diode but an old 1N34 removed years ago from a 1950s-era Heathkit has given it a good run for the money! I've still several hundreds of early germanium diodes, pulled from old diode matrix boards years ago, to test against the D18 as well as numerous Schottky diodes.

Also on board the detector module is a Selectivity Enhancement Circuit (SEC) that increases selectivity by unloading some of the diode's effect on the detector coil, similarly to tapping the diode further down the tank coil. It uses a small butterfly capacitor seen to the right of the main tuning capacitor in the photo above. I found it extremely effective when needed and is well worth the addition to a high-performance tuner.

The detector stage is followed by an impedance-matching transformer for the sound-powered headphones. This stage also houses a 50uA meter to measure diode current / signal strength levels.



 

 

The meter can be switch-bypassed to prevent needle-bounce on stronger signals. It is particularly helpful when using the traps to null a signal to the minimum level.

 

 

The three traps utilized have been very effective in eliminating what I had originally perceived as an impossible DXing situation.

Here are the daytime-power signal strengths of my 15 line-of-site blowtorch stations that, without trapping, very effectively block most sections of the band. Anything over 50uA is ear shattering and problematic, usually requiring the use of all 3 traps:

             KVRI 1600 50uA
             KRPI 1550 100uA
             CJVB 1470 40uA
             CFTE 1410 350uA
             CHMB 1320 100uA
             CJRJ 1200 400uA
             CKWX 1130 300uA
             CKST 1040 90uA
             CKNW 980 150uA
             KGMI 790 100uA
             CHMJ 730 450uA
             CBU 690 650uA
             CISL 650 200uA
             CKSP 600 100uA
             KARI 550 100uA

Overall I was very pleased and surprised at the good performance of the new radio. During the contest period I identified and logged 92 unique stations in 16 states / provinces. More than one station was logged on 9 different frequencies as the propagation varied from night to night.

Highlights of the DX Contest were hearing WHAS in Kentucky (2,007 miles), WJR in Michigan (1,970 miles), KXEL in Iowa (1,556 miles), WCCO in Minnesota (1,423 miles) and CBW-990 in Winnipeg, smack up beside local blowtorch CKNW-980! Additionally, hearing Washington state 250 watter KFLD-870 and 250 watt KWBY-940 in Oregon were great surprises.


I found the use of a spotter radio (Sony ICF-2010) to be very useful in locating signals to target and to zero-beat with an RF signal generator. The generator’s tone-modulated signal can then be tuned in and the xtal radio and antenna / detector stages optimized. 

From here, any pest signals are then tuned to and individually nulled using the traps while watching the signal meter. Antenna and detector stages are then re-tweaked before disabling the generator and listening for the desired signal. 

Often it is heard immediately following the above tuning procedures but if not, monitoring the frequency for several minutes often allows time for the weak signal to fade up to audible levels. 

Comparing programming audio with what is heard on the spotter radio will confirm hearing the correct signal as will comparing audio to the station’s own live-feed on the internet.


Due to the larger and much better antenna (inverted-L 70’ x 100’) on the crystal radio, I would often hear good audible signals on it and not on the spotter (something that I found surprising) so often times it was productive to just tune around the band on the crystal radio, tweaking stages as required.


I’m looking forward to further improvements of the tuner as well as to the next DX Contest whenever that will be scheduled ... hopefully you can join in as well!

 
CONTEST LOG (pests in red)

                    FREQ UTC    STN    LOCATION    MI      

540    3:50    CBK    Watrous, SK    764      
550    1:04    KARI    Blaine, WA    25      
560    1:30    KPQ    Wenatchee, WA    168      
570    3:45    KVI    Seattle, WA    107      
580    3:42    KIDO    Nampa, ID    492      
600    1:17    CKSP    Vancouver, BC    32      
610    4:15    KONA    Kennewick, WA    271      
620    1:22    KPOJ    Portland, OR    241      
630    3:40    CHED    Edmonton, AB    530      
630    21:10   KCIS    Edmonds, WA    87      
650    1:05    CISL    Richmond, BC    24      
660    3:30    CFFR    Calgary, AB    693      
660    21:23   KAPS    Mt. Vernon, WA    52      
670    3:25    KBOI    Boise, ID    807      
690    1:06    CBU    Vancouver, BC    19      
710    3:21    KIRO    Seattle, WA    108      
730    1:02    CHMJ    Vancouver, BC    22      
750    3:55    KXTG    Portland, OR    243      
760    4:01    WJR    Detroit, MI    1970      
770    3:17    KATL    Miles City, MT    831      
780    4:00    KKOH    Reno, NV    658      
790    1:07    KGMI    Bellingham, WA    39      
810    4:05    KGO    San Francisco, CA    786      
820    1:59    KGNW    Seattle, WA    106      
830    2:20    WCCO    Minneapolis, MN    1423      
840    4:10    CFCW    Camrose, AB    530      
840    4:00    WHAS    Louisville, KY    2007      
850    4:20    KOA    Denver, CO    1118      
850    1:12    KHHO    Seattle, WA    121      
860    3:48    CBKF    Saskatoon, SK    758      
860    1:04    KPAM    Troutdale, OR    226      
870    4:30    KFLD    Pasco, WA    266      
880    1:17    KIXI    Seattle, WA    102      
890    4:35    CJDC    Dawson Creek, BC    494      
900    4:38    CKBI    Prince Albert, SK    810      
910    4:40    CKDQ    Drumheller, AB    468      
920    4:42    KXLY    Spokane, WA    285      
930    1:50    KBAI    Bellingham, WA    37      
940    4:45    CJGX    Yorkton, SK    940      
940    0:58    KWBY    Woodburn, OR    256      
950    4:50    KJR    Seattle, WA    106      
960    4:52    CFAC    Calgary, AB    444      
970    4:55    KBUL    Billings, MT    722      
980    1:08    CKNW    New Westminster, BC    32      
990    4:58    CBW    Winnipeg, MB    1156      
1000  3:45    KOMO    Seattle, WA    105      
1010  4:59    CBR    Calgary, AB    453      
1020  0:54    KWIQ    Moses Lake, WA    216      
1030  5:06    KTWO    Casper, WY    918      
1040  1:09    CKST    Vancouver, BC    23      
1050  5:10    CJNB    N Battleford, SK    707      
1060  5:07    CKMX    Calgary, AB    441      
1070  5:10    cfax    Victoria, BC    33      
1080  0:33    KFXX    Portland, OR    232      
1090  1:40    KFNQ    Seattle, WA    109      
1100  3:55    KFAX    San Francisco, CA    779      
1110  5:15    KRPA    Oak Harbor, WA    48      
1120  0:48    KPNW    Eugene, OR    340      
1130  1:10    CKWX    Vancouver, BC    22      
1140  5:20    CHRB    High River, AB    443      
1150  5:50    CKFR    Kelowna, BC    185      
1160  5:53    KSL    Salt Lake Cty, UT    781      
1170  1:11    KPUG    Bellingham, WA    39      
1180  5:09    KOFI    Kalispell, MT    416      
1190  5:55    KEX    Portland, OR    241      
1200  1:12    CJRJ    Vancouver, BC    23      
1260  5:58    CFRN    Edmonton, AB    522      
1290  6:00    KUMA    Pendleton, OR    306      
1290  6:00    KGVO    Missoula, MT    449      
1320  1:13    CHMB    Vancouver, BC    23      
1360  6:12    KKMO    Tacoma, WA    115      
1370  4:32    KXTL    Butte, MT    535      
1380  6:16    KRKO    Everett, WA    88      
1410  1:14    CFTE    Vancouver, BC    22      
1460  1:55    KUTI    Yakima, WA    207      
1470  1:15    CJVB    Vancouver, BC    25      
1480  1:20    KBMS    Vancouver, WA    227      
1520  1:05    KKXA    Snohomish, WA    88      
1520  1:13    KQRR    Oregon City, OR    241      
1530  4:30    KFBK    Sacramento, CA    698      
1540  1:50    KXPA    Bellvue, WA    102      
1540  4:46    KXEL    Waterloo, IA    1556      
1550  1:16    KRPI    Ferndale, WA    31      
1560  1:14    KVAN    Burbank, WA    272      
1580  6:25    KGAL    Lebanon, OR    297      
1590  1:22    KLFE    Seattle, WA    91      
1600  1:00    KVRI    Blaine, WA    25      
1620  1:30    KYIZ    Renton, WA    111      
1640  6:45    KDZR    Lake Oswego, OR    239      
1660  0:56    KBRE    Merced, CA    812      
1680  1:35    KNTS    Seattle, WA    91      
1690  0:53    KFSG    Roseville, CA    705     


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