[ARC5] Crystal Headphones
Richard Knoppow
1oldlens1 at ix.netcom.com
Tue Sep 18 17:33:57 EDT 2018
One must be careful not to confuse sensitivity with the
impedance. Sensitivity is a power measurement, that is electrical
power in to acoustical power out. It is possible to have high
impedance but low power sensitivity although I can't give you an
example of a commercial headphone. High impedance is desirable
for sources that are high impedance such as crystal sets and AC
impedance bridges. However, where the source is low or medium
impedance headphones with matching impedance will be louder than
the high impedance phones. Testing for sensitivity requires a
calibrated artificial ear if the results are to have any
accuracy. These are rare. However, one can test with just your
ears or a sound level meter with the microphone held against the
headphone. An interesting experiment is to take an oscillator and
feed various headphones from it through a very high value
resistor, preferably at least five times the expected headphone
impedance. 100K is enough although more is better. Just connect
the phones and see which is the loudest. Usually, it will be the
ones with the highest impedance but some with the same impedance
will differ. In some cases a lower impedance phone will be louder
than a higher impedance one. The difference is probably in the
magnet strength but can also be due to differences in the
diaphragm spacing from the pole pieces.
The loudest phones I have are: Western Electric 509W, WE
Signal Corps P-11, Baldwin Type C. However, if you make the same
test using a low impedance source, say 500 ohms, the results will
be different. For instance WE type 528 (600 ohm) will be louder
than the WE 509W. WE and Trimm made magnetic phones down to about
50 ohms per pair. For the same reason you may find modern
high-fidelity moving coil phones too loud when connected to a
receiver where they are across the loudspeaker output. Typically,
this will be 4 to 8 ohms and most of these phones are are around
50 ohms impedance. The receivers will often specify 500 ohms
although 20K phones usually work just fine and are of reasonable
loudness.
Measuring efficiency is a matter of measuring power out to
power in. That requires an impedance match on the electrical side
and, for best power efficiency, also on the acoustical side.
Most of the magnetic type phones have a strong resonance,
typically in the vicinity of 1Khz. While some attempt was made to
broaden out the resonance (such as using a salt shaker type cap)
the difference is not great. It is possible to make quite non
resonant magnetic phones but they become complex. The best
example is the Western Electric type HA-2 designed for the series
500 telephone. These are described in great detail in the Bell
System Technical Journal and elsewhere by Mott and Miner of Bell
Labs who designed it. There are other types that fall broadly in
the "magnetic" category, such as the balanced armature type as
typified by the Baldwin phones with mica diaphragms and also used
in some sound-powered phones.
While one can find oodles of information about moving coil
speakers and microphones in the technical literature of the last
century there is not much about the plain magnetic phones
although they were made by many different companies. Frustrating.
FWIW, the highest impedance phones magnetic phones I've
measured are the WE SC type P-11 (close to 30K), others were the
WE 509W (25K), Trimm Featherweight (24K) but the Featherweights
are not as loud on a very high impedance source as the WE phones
or as the Trimm Commercial phones which measure only 17K
(advertised value).
Measurements were made on: General Radio 650A bridge with
external null detector, GR 1650A, GR Z-Y bridge, all at 1K
Note also that magnetic phones are mostly inductive so the
impedance varies with the frequency. I measure at 1K. I found the
advertised values of Trimm phones are high at 1K but about right
at 1200 Hz. However, the resonance is at about 1K. I tried to
measure the motional impedance of a couple of phones but gave it
up because I can't separate it from the overall impedance. i.e.,
you can't see a resonant rise in the impedance.
Enough, I am glad at least one or two people find this of
some interest.
On 9/18/2018 1:35 PM, Dennis Monticelli wrote:
> More modern magnetic phones (still of the old style) can be quite
> good.
>
> I have a NIB set of H-43B/U headphones (datecode 1990) that were
> made for Geiger counters. I measured an impedance of 21K at 1KHz
> so I presume the transducers are 10K wired in series. These cans
> produce plainly audible tones with only 1mV rms. That equates to
> 50 picowatts! Impressive sensitivity and high enough Z for
> crystal radios.
>
> Dennis AE6C
--
Richard Knoppow
1oldlens1 at ix.netcom.com
WB6KBL
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