An 'S' meter, for a crystal radio with high-impedance phones, is generally a high-resistance microammeter connected across the phones. In other words, a sensitive voltmeter that does not bypass headphone current significantly.
![](https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEhYNswP8Vz8TAnlD2TTznFTQwVTbfFMcc6Or77r8N52XhTYkSB4LZBpiQdmyexiHDU88lX6zj1X_FGSDobm7h4kkqHbHUUl0WtM-c9jlpvvfUQmFLt3NVFV5sp1hXyj8RNWprojSQ9zppM/s200/1.JPG) |
Crystal Radio 'S' Meter |
On the other hand, for a crystal radio with low-impedance phones, it's a low resistance microammeter connected in series with the phones. That is, a sensitive ammeter that does not drop headphone current significantly.
A voltmeter, discovered in my junk box, was used to build such a meter for my crystal radio which uses low-impedance balanced-armature phones.
![](https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEjXL12_cHwHL6FEM3_SPqUM33hZtq3K6dMi1HbzqYzQmkTOLtPPN6Vu6VpF4ciSyTAdH4zPgIpElSqQDrQe0QfifIXifV9_WlkQUG85zGmWQ7yhWZYLDKPPpWIDPBJQQ5TQ5bphnW_WVv5H/s200/untitled.JPG) |
Crystal Radio 'S' Meter - Schematic |
On removing its series and shunt resistors, the resistance of the 1 mA FSD movement turned out to be only 60 Ω and hence quite suitable for the purpose. The existing graduations on the meter face were removed and replaced with graduations 0 -10 using a lead pencil.
The meter was already mounted on a square bakelite flange. The flange mounting holes served as terminal mounting holes, obviating the need for an enclosure.
The result - an interesting weekend project and a handy crystal radio test aid.
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