Here is an entirely different way to calibrate the magnetic field in a Helmholtz coil.
This method uses an integrating opamp and a coil inserted in the magnetic field to integrate the field when the coil is flipped end-to-end. Use an integrating coil (flip-coil) which is based on Faraday’s law in integral form:
∫V·dt = -N·B·A volt-seconds
Here A is area of coil, N is number of turns, B is magnetic field, and ∫V·dt is the output. The coil is placed in the magnetic field B, and the coil is flipped (end-to-end), so the total volt-seconds is 2·N·B·A. Alternatively, for a Helmohtz coil, the current can be turned off or reversed, but this will not measure the Earth’s field contribution to B.
A circuit for measuring the volt-seconds is shown in the attachment. For the circuit shown, the opamp output voltage Vout is, using standard opamp equations and Faraday’s Law (above):
Vout = [1/(R1·C1)] ∫V·dt = - N·B·A/(R1·C1) volts (see attachment for R1 and C1)
Example:
Wind 500 turns of thin (30 Ga. Or thinner) enameled copper wire on a 3-cm diameter coil form. For a 100 Gauss field, NBA = 500 turns x 0.01 Tesla x 7.069 x 10-4 m2 = 3.53 x 10-3 volt seconds.
If R1 = 10 k, and C = 0.1 uF as shown in the attachment (R1·C1 = 0.001 seconds),
and if the coil is flipped in a 100-Gauss field (Helmholtz coil field), the voltage output of the circuit is
Vout = 2 N·B·A/.001 = 7.06 volts, or to measure the field:
B = R1·C1·Vout/(2·N·A) Tesla
An operational amplifier with a low input offset voltage and a low input offset current should be used. The integrating capacitor should be a high quality, bipolar, low leakage capacitor. If necessary, the opamp leakage current can be nulled using a 10-meg resistor into the summing junction from a potentiometer -1 volt< V <+1 volt.
For general integrator construction, use a DIP package from Analog, National, or Linear with low voltage and cbias current offsets and low temperature drift characteristics.
This is an absolute magnetic field calibration, and depends only on the size of the integrating coil NA, and the R1 C1 product.
Bob S
[added] The resistance of the flip coil should be included in the value for R1. For the example I gave above, a 30-Ga wire coil would add about 15 ohms to R1. R1 is selected to equalize the effect of the input offset voltage and the input offset current in a typical opamp. Both can be zeroed out with a potentiometer.