A number of people noticed my comment on having the electrical schematics for the Extech LCR meter, and expressed interest. Accordingly, I have added the schematics to my website Joe Gwinn's website homepage.
No Principles-of-Operation text has been found, but I did work out how it works. I described the basic approach in a posting on the effect of eddy currents on inductance. Specifically message #44 of http://music-electronics-forum.com/t14110-2/#post113076.
Here is the relevant text from posting #44:
I found the circuit diagram of the Extech (under a different brand name) on the web. For the record, it measures in the following way:
The 1000 Hz (or 120 Hz) oscillator has two outputs, one at 0 degrees (I) and one at 90 degrees (Q) phase shift. The 0 degrees output is amplified and imposed on the unit under test (UUT), a pickup in this case. Both 0 and 90 degree outputs are fed to a pair of synchronous demodulators, as will be discussed later.
The voltage across the UUT is sensed by one opamp circuit, and the current through the UUT is sensed by another opamp circuit, yielding two voltage signals, one proportional to UUT voltage and the other to UUT current.
These two voltages are fed one at a time to to the pair of synchronous demodulators, yielding a pair of complex numbers.
The first complex number consists of the I (real) and Q (imaginary) values of the UUT voltage, and the second complex number consists of the I and Q values of the UUT current.
The complex impedance (I and Q) is the UUT voltage (I and Q) divided by the UUT current (I and Q).
Not mentioned above is one practical complication, a circuit that compensates for the non-zero input impedance of the current-to-voltage converter.
No Principles-of-Operation text has been found, but I did work out how it works. I described the basic approach in a posting on the effect of eddy currents on inductance. Specifically message #44 of http://music-electronics-forum.com/t14110-2/#post113076.
Here is the relevant text from posting #44:
I found the circuit diagram of the Extech (under a different brand name) on the web. For the record, it measures in the following way:
The 1000 Hz (or 120 Hz) oscillator has two outputs, one at 0 degrees (I) and one at 90 degrees (Q) phase shift. The 0 degrees output is amplified and imposed on the unit under test (UUT), a pickup in this case. Both 0 and 90 degree outputs are fed to a pair of synchronous demodulators, as will be discussed later.
The voltage across the UUT is sensed by one opamp circuit, and the current through the UUT is sensed by another opamp circuit, yielding two voltage signals, one proportional to UUT voltage and the other to UUT current.
These two voltages are fed one at a time to to the pair of synchronous demodulators, yielding a pair of complex numbers.
The first complex number consists of the I (real) and Q (imaginary) values of the UUT voltage, and the second complex number consists of the I and Q values of the UUT current.
The complex impedance (I and Q) is the UUT voltage (I and Q) divided by the UUT current (I and Q).
Not mentioned above is one practical complication, a circuit that compensates for the non-zero input impedance of the current-to-voltage converter.
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