Product Description

The broadband induction coil magnetometer MFS-07e has been developed to measure variations of the Earth´s magnetic field, particularly for applications in Magnetotellurics (MT) and Controlled Source Audio Magnetotellurics (CSAMT). It covers a wide frequency range from 0.001 Hz up to 50 kHz. In spite of its broad bandwidth, the MFS-07e shows outstanding low-noise characteristics, extremely low temperature drift of input offset voltage and offset current and a very stable transfer function over temperature and time. The MFS-07e is the result of many years of experience of metronix in the design, manufacture and application of induction coil magnetometers. As a unique feature the MFS-07e acts as an “intelligent plug and play” sensor. Thus, once connected to the ADU-07e, it will send its type and serial number as well as its calibration function to the ADU-07e automatically. The user does not have to care about any further sensor parameter setup.

metronix magnetometers have been used by numerous customers throughout the world - including geophysical exploration companies and research institutes.


A complete magnetic field measurement site consists of three single axis orthogonal sensors. Each sensor is enclosed in a shock resistant cylindrical tube that acts as a protection against mechanical stress. These tubes are waterproof and also resistant to ultraviolet radiation. The magnetometer contains the electronics for pre-amplification of the weak sensor signal as well as for precise self calibration. The MFS-07e magnetometer is connected to the metronix ADU-07e data logger (or any other custom electronics) by a cable of up to 70 m in length. Special care is taken to the fact that magnetometers are often used under rough environmental influences. All cables have ruggedized waterproof connectors. The very high quality of the MFS-07e data is achieved by a unique design for the ultra low noise and low frequency preamplifier.


The MFS-07e has several outstanding features which make it a first class instrument for the electromagnetic exploration:

  • Wide frequency range from 1/1000 Hz to 50 kHz covered by only one sensor

  • High linearity

  • Ultra low noise

  • High accuracy calibration with built-in precision calibration facility

  • Wide operating temperature range from -25° C to +70° C

  • high stability of the sensor´s transfer function due to magnetic field feedback

  • built-in signal amplification and conditioning electronics

  • Metronix “Smart Sensor” technology – sensor parameters incl. transfer function can be read by ADU-07e automatically

  • easy field handling and small measures

Technical Data

Frequency range

0.001 Hz ….. 50 kHz

Frequency bands

0.001 Hz ….. 500 Hz (chopper on), 10 Hz ….50 kHz (chopper off)

10 Hz ….10 kHz (chopper off)

Sensor noise

3*10-2 nT/√Hz @0.01 Hz

3*10-4 nT/√Hz @1 Hz

5*10-7 nT/√Hz @ 1000 Hz (chopper off)

Output sensitivity

0.02 V/(nT*Hz) f<< 32Hz

0.64 V/nT f>> 32Hz

for exact values refer to individual calibration file

Output voltage range

+/- 10V


induction coil with magnetic field feed back


10 pole ODU Series K

Calibration coil sensitivity

1.6 nT / V

Feedback cut-off frequency

32 Hz

Supply voltage

+/- 12V to +/-15V stabilised and filtered

Supply current

+/- 25mA


ruggedized, waterproof case


ca. 6 kg

External dimensions

length 710 mm incl. cap, diameter 75mm

Operating temperature range

-25°C ….. + 70°C


The central part of the MFS-07e magnetometer is the sensor coil. It consists of a high permeable ferrite core and several thousand turns of copper wire. Due to its low skin depth the core material prevents the occurrence of eddy currents in the measurement frequency range.

To achieve good mechanical stability the main structure of the sensor is based on the cylindrical tube which is made of fibre glass reinforced epoxy.

Induction coil sensors do not measure the magnetic field itself but its time derivative. This is expressed in the law of induction:

\(V_{ind} = n \cdot \frac{d\Phi}{dt}\)



induction voltage


number of turns


magnetic flux

The flux \(\ \Phi\) which flows through one loop of the coil is calculated as

\(\ \Phi = B \cdot A = \mu_{0} \cdot \mu_{c} \cdot H \cdot A\)



magnetic flux density parallel to the sensor axis


permeability constant


permeability of the core


cross section of the core


magnetic field amplitude \((= \hat{H} \cdot e^{j\omega t})\)



For a sinusoidal magnetic field which can be written with a phasor as \(\overset{\sim}{H} = \hat{H} \cdot e^{j\omega t}\) the induced voltage of the sensor output becomes

\({\overset{\sim}{V}}_{ind} = {\hat{V}}_{ind} \cdot e^{j\omega \cdot t} = j \cdot \underset{S_{0}}{\underbrace{2\pi \cdot n \cdot \mu_{0}\mu_{c} \cdot A}} \cdot f \cdot \hat{H} \cdot e^{j\omega \cdot t} = j \cdot f \cdot S_{0} \cdot \overset{\sim}{H}\)

\(S_{0}\) is defined as the sensor’s sensitivity constant which gives the relation between the magnetic field’s amplitude and the induction voltage. This equation is only a theoretically one. A non ideal sensor’s equivalent circuit does not only contain the field proportional voltage source (which itself is not really proportional) but also some further elements:


Simplified equivalent circuit diagram for a sensor coil

Referring to the source, the induced sensor voltage \(V_{ind}\), the coil resistance \(R\), the input resistance of the amplifier \(R_{d}\) the coil inductivity \(L\) and the capacity \(L\) yield a damped serial resonance circuitry. The transfer function of the sensor will show a strong peak at its resonance frequency.

For the sensor itself, without the preamplifier, we get the transfer function

\(\frac{V_{e}}{V_{ind}} = \frac{\left. {R_{d}/\left( R_{d} + R \right.} \right)}{1 - \left( f/f_{0})^{2} + j \cdot 2D \cdot \left( f/f_{0} \right) \right.}\)

with the amplifier’s input resistance \(R_{d}\), Gain \(G\), resonance frequency \(f_{0}\) and attenuation \(D\) defined as

\(f_{0} = \frac{1}{2\pi \cdot \sqrt{a \cdot L \cdot C}}\) \(~a = \frac{R_{d}}{R + R_{d}}\) \(G = \frac{V_{M}}{V_{e}}\) \(2D = \sqrt{\frac{R_{d}}{R_{d} + R}} \cdot \frac{\sqrt{L/C}}{R_{d}} + \frac{R}{\sqrt{L/C}}\)

Having this in mind the resulting transfer function between the magnetic field and the sensor output voltage becomes

\(F_{sensor} = \frac{\hspace{0pt}\hspace{0pt}\hspace{0pt}V_{e}}{\overset{\sim}{H}} = \frac{j \cdot S_{0} \cdot {R_{d}/\left( R_{d} + R \right)} \cdot f}{1 - \left( f/f_{0})^{2} + j \cdot 2D \cdot \left( f/f_{0} \right) \right.}\)

The equivalent circuit diagram of the magnetometer leads to a frequency dependent sensitivity \(E(f)\) referred to the preamplifier output of:

\(E\left( f \right) = E_{0} \cdot \frac{V_{e}}{V_{ind}}\)


\(E_{0} = G \cdot S_{0}\)


Relative frequency response of magnetometer MFS-07e for \(H(f) = const\).

Figure 2-2 shows the principle frequency response of the output voltage \(V_{m}\) of the MFS-07e. Considering the feedback, the output voltage is given by:

\(V_{M}\left( f \right) = \frac{j \cdot f \cdot H\left( f \right) \cdot E\left( f \right)}{1 + j\frac{f}{f_{c}}}\)

The cut-off frequency of the magnetometer is set to \(f_{c} = 32Hz\).

Please consider that this figure shall only explain the feedback principle. Additional effects caused by the low-pass filtering of the sensor signal at \(40 kHz\) and other influences are not respected here.


The integrated preamplifier performs the signal amplification of the sensor output voltage as well as the conditioning of the magnetic field feedback signal and allows to feed-in an external calibration signal. Special care has been taken to avoid disturbance of the electronics by external electromagnetic noise.

To achieve DC characteristics close to the physical limits, the preamplification electronics is split into a lower frequency path (low-pass corner frequency \(330 Hz\)) which is chopper stabilized in order to achieve excellent low-noise and drift characteristics and a separate AC path with the same corner frequency. The output signals of these two amplification paths are used as an input for the magnetic feedback conditioning stage.

The following block diagram explains the design:


MFS-07e block diagram

The resulting frequency characteristics of the MFS-06e sensor system is dominated by the feedback loop. As it was demonstrated in chapter 2 of this manual, the characteristics of the sensor itself mostly depends on the resonance circuit formed by the main impedance and main capacity of the coil. This leads to a strong peek in the spectrum at the resonance frequency \(f_{0}\).

In the block diagram above the summing function for the input node leads to the transfer function, assuming that \(U_{pre}\) is the output voltage of the amplifier input stage:

\(\left( H - U_{pre} \cdot F_{FB} \right) \cdot F_{sensor} \cdot F_{amp\_ in} = U_{pre}\)

which is the same as

\(\frac{U_{pre}}{H} = \frac{1}{\left( F_{sensor} \cdot F_{amp\_ in} \right)^{- 1} + F_{FB}}\)

Close to the resonance frequency the influence of the sensor transfer function disappears and the overall characteristics depends mainly on \(F_{FB}\). This results in a flat frequency response of the sensor system over the whole frequency band of interest.

Additionally the preamplifier electronics contains an output line driver which provides an \(40 kHz\) low-pass filter. The output buffer is able to drive cables up to 70 m length.


Preamplifier of MFS-07e

Transfer Function of MFS-07e

The transfer function of the MFS-06e magnetometer is determined by the transfer function of the preamplifier, the feedback electronics and the sensor transfer function.

The theoretical overall transfer function is defined by the following equations:


\(F_{Sensor} = \frac{V_{output}}{H} = 0.64\frac{V}{nT} \cdot \frac{P_{1}}{1 + P_{1}} \cdot \frac{1}{1 + P_{2}} \cdot \frac{1}{1 + P_{4}}\)

or normalized as we use it in our calibration files:

\(F_{on}(f) = \frac{ V_{output} }{H \enspace Hz} = 0.64 \frac{V}{nT} \cdot \frac{P_1}{1+P_1} \cdot \frac{1}{1+P_2} \cdot \frac{1}{1+P_4} \enspace / \enspace f\)


adds a term \(P_3 = i \frac{f}{0.72 Hz}\)

\(F_{Sensor} = \frac{V_{output}}{H} = 0.64\frac{V}{nT} \cdot \frac{P_{1}}{1 + P_{1}} \cdot \frac{1}{1 + P_{2}} \cdot \frac{P_{3}}{1 + P_{3}} \cdot \frac{1}{1 + P_{4}}\)

or normalized as we use it in our calibration files:

\(F_{off}(f) = \frac{ V_{output} }{H \enspace Hz} = 0.64 \frac{V}{nT} \cdot \frac{P_1}{1+P_1} \cdot \frac{1}{1+P_2} \cdot \frac{P_3}{1+P_3} \cdot \frac{1}{1+P_4} \enspace / \enspace f\)


\(P_{1} = i \cdot \frac{f}{32Hz}\), \(P_{2} = i \cdot \frac{f}{40000Hz}\), \(P_{3} = i \cdot \frac{f}{0.72Hz}\), \(P_{4} = i \cdot \frac{f}{50000Hz}\)


Hence that below 100 Hz chopper should be really on.

This theoretical transfer function is only an approximation of the real transfer function (approx. up to \(500 Hz\) with Chopper On) which is delivered by the calibration of the sensor. Each sensor is delivered with a calibration file which has a 3 column ASCII format. The left column represents the frequency, the middle one represents the sensor sensitivity in \(\frac{V}{nT \cdot Hz}\) and the right one the phase in degree.

As it can be easily calculated from the equation above, for very low frequencies the transfer function of the coil converges to \(\frac{0.2V}{nT \cdot Hz}\) in amplitude and to 90 degrees in phase. The calibration data which is delivered along with the coil ends at its low end at \(f = 0.1 Hz\). The amplitude can be taken as the given value at \(0.1 Hz\) also for lower frequencies. The phase value for very low frequencies \(<0.1Hz\) can be computed to

\(\varphi = atan\left( \frac{32Hz}{f} \right)\) with \(f < 0.5Hz\)

Additionally to the calibration file the sensor is equipped with the calibration data stored on a chip inside the sensor. This information will be read by the ADU-07e. Each time a data recording is done this calibration data is stored along with the recording data.

Integrated Calibration Facility

The integrated calibration facility makes it easy for the user to perform an online calibration or test of the magnetometer transfer function. A differential test signal can simply be injected into the CAL inputs and is internally added to \(U_{pre}\) without further amplification as shown in Figure 3-1. A voltage on the CAL input results in a magnetic field according to

\(H = 1.6\frac{nT}{V} \cdot U_{cal}\)

This makes it easy to calculate the resulting transfer function of the magnetometer using the formula

\(F_{MFS - 07e} = \frac{U_{out}}{U_{cal}} \cdot \frac{1}{1.6\frac{nT}{V} \cdot f}\)

External magnetic field variations do not disturb the measurement if a correlation analyser (e.g. Solartron 1250) is used. The input signal must be in the range of \(\pm 10V\) peak to peak.

If the metronix ADU-07e is used as data logger the magnetometer characteristics will be tested regularly as a part of the normal system self test.

Calibration by Manufacturer

metronix takes special care of the initial calibration of all MFS-06e magnetometers as part of the ISO9001:2008 certified production process. Tests have demonstrated an excellent long time stability of the transfer function.

The calibration is performed in the „Magnetsrode“ geomagnetic laboratory which is operated by the Institute of Geophysics at the Technical University of Braunschweig, mostly to calibrate space flight magnetometers. It offers special environmental circumstances and has an extremely low distortion level.

A large solenoid (l = 3.6 m; d = 30 cm) has been calibrated by a reference sensor with an accuracy of better than ±0.2%. It is used to generate a homogeneous magnetic field of known strength as input signal. The input signal for the solenoid comes from a N4L PSM3750 phase sensitive multimeter which is able to perform calculation of transfer functions with a given statistical accuracy.

Each magnetometer is calibrated to a sensitivity

\(E = 0.02\frac{V}{nT \cdot Hz}\)

at a frequency of 0.4 Hz.

A calibration file is generated in a frequency range between 0.4 Hz and 60 kHz. Lower frequency calibration is not required because the sensor obeys the mathematical rules (theoretical transfer function with a very high precision.

Table 0-1 gives an example of a calibration file delivered along with the sensor. Note that not all calibration results are given here due to limited space, gaps are marked by dots here.

Each magnetometer is shipped with the original calibration data set which contains the measured values of amplitude and phase of the transfer function over the specified frequency band.

The calibration file is split into 2 sections first section with the chopper switched on, 2nd section with the chopper switched off.

Figure 6-1 and Figure 6-2 show the plots of the calibration function of MFS-07e Ser. #002.


Typical sensitivity calibration curve of MFS-07e


typical phase calibration curve of MFS-07e

  Calibration measurement with NumetriQ PSM 3750 - 0.1.100000.1.17

Metronix GmbH, Kocherstr. 3, 38120 Braunschweig

Magnetometer: MFS07e#389 Date: 15/04/20 Time: 07:37:32

Hz V/(nT\*Hz) deg
Chopper On

+4.0000E-01 +1.9976E-02 +8.9270E+01
+5.5579E-01 +1.9907E-02 +8.8983E+01
+7.7227E-01 +1.9985E-02 +8.8612E+01
+1.0731E+00 +1.9943E-02 +8.8080E+01
       .            .            .
       .            .            .

+2.0718E+04 +2.2497E-05 -7.6792E+01
+2.8787E+04 +1.3224E-05 -9.7165E+01
+4.0000E+04 +7.5303E-06 -1.2228E+02
+5.5580E+04 +4.0556E-06 -1.5603E+02
+6.0000E+04 +3.3949E-06 -1.6478E+02

Chopper Off
+4.0000E-01 +1.0758E-02 +1.4764E+02
+5.5579E-01 +1.3267E-02 +1.3882E+02
+7.7227E-01 +1.5700E-02 +1.2904E+02
+1.0731E+00 +1.7671E-02 +1.1983E+02
       .            .            .
       .            .            .
+2.8787E+04 +1.3161E-05 -9.7254E+01
+4.0000E+04 +7.5026E-06 -1.2229E+02
+5.5580E+04 +4.0453E-06 -1.5611E+02
+6.0000E+04 +3.3797E-06 -1.6481E+02

Example for a calibration file (the dots indicate that not all lines are shown here)

Sensor Noise

In an electromagnetic measurement system special care has to be taken to noise. The various sources of noise in the system can be referenced back to an equivalent input noise voltage at the preamplifier input for comparison purpose which is expressed in the equation

\(\sqrt{\frac{\overset{¯}{u^{2}}}{\Delta f}} \approx \sqrt{\frac{\overset{¯}{u_{amp}^{2}}}{\Delta f} + \frac{\overset{¯}{u_{R}^{2}}}{\Delta f} + \frac{\overset{¯}{i_{amp}^{2}}}{\Delta f} \cdot \left( \omega^{2}L^{2} \right)}\)



preamplifier noise voltage density (typ. \(1.6nV/\sqrt{Hz}\))


thermal noise of sensor resistance (typ. \(1.6nV/\sqrt{Hz}\))


preamplifier noise current density (typ. \(10fA/\sqrt{Hz}\)) @chopper off

To rereference this noise voltage back to the magnetic field the formula

\(\sqrt{\frac{\overset{¯}{H^{2}}}{\Delta f}} = \frac{\sqrt{\frac{\overset{¯}{u_{}^{2}}}{\Delta f}}}{E_{o} \cdot f} = \frac{1nT}{6.6\mu\;V/\sqrt{Hz} \cdot f} \cdot \sqrt{\frac{\overset{¯}{u_{}^{2}}}{\Delta f}}\)

is used. These two equations show that the current noise is spectrally flat whereas the voltage noise of the amplifier and the coil resistance increase proportional with 1/f to low frequencies. For higher frequencies it is possible to eliminate a part of the preamplifier noise if the chopper path is switched off. This can be done with a pulse on the HCHOP line.

Magnetometer noise is measured at metronix with an HP spectrum analyser. To keep environmental noise away from the sensor the measurements are done with the magnetometer in a multiple shielded Mu-metal chamber.

Additionally, the noise of the magnetometer is measured by a parallel sensor test. The correlation between two parallel located sensors is determined and by this means, in connection with the measured amplitude spectra, the noise of the sensor can be computed.


Installation of Magnetometers

To avoid low frequency distortion due to mechanical vibrations of the sensor it must be dug into the soil. If this is not done, significant noise caused by wind may be created which can make a measurement unusable. The z component magnetometer should be dug into the soil at least to the amount of half of its size. In order to obtain optimum results the free end of the sensor should be covered by a protection cap like a plastic bucket.

Special care must be taken to the exact alignment of the magnetometer tube. It’s bottom side (that one without the cable connector) must point exactly to the corresponding (positive sensor) direction:

  • X magnetometer to the North

  • Y magnetometer to the East

  • Z magnetometer to the ground

A positive flux change in the positive sensor direction will cause a positive change in the output voltage.

Electrical Connection

All magnetometer cables from metronix are shielded twisted pair cables which perform optimum protection against external distortion. Connectors have best outdoor characteristics including water tightness. Nevertheless, care should be taken to avoid intrusion of particles. Each connector has a protection cap which can be removed by just pulling it off. Please ensure that the expensive connectors are always protected by the caps during assembling or disassembling of the MT system.

To connect a cable to a magnetometer rotate it to the coded position (red dot to red dot), put connector into the input plug and lock it by pushing it until it snaps in.

The MFS-07e can be directly connected to the ADU-07e data logger. Due to the easy setup procedure of a metronix GMS-07 system, the magnetometer cables simply have to be put into the corresponding ADU-07 ports.

In case other custom electronics is used the production of a suitable cable connection should be not too difficult according to the pin assignment given below.


Special care must be taken with custom electronics to avoid a wrong use of the power supply inputs! The magnetometer electronics may be damaged immediately if the power is connected the wrong way!


The Chopper On/Off Signal is a standard CMOS input. Low level (<0.5V) will switch the chopper amplifier off. High level (>3.5V up to 13V) will switch the chopper on. If you use the sensor with custom electronics, make sure to switch the chopper line on and off with a delay of about 100ms or more in order to properly initialize the sensor.

Installation with ADU-07e

This chapter describes the setup of the MFS-07e in the field in connection with the ADU-07e.

Standard 5-channel MT Setup

Figure 0-1 illustrates the field setup of a five channel MT station. Only a few components are required:

  • ADU-07e with battery and GPS antenna

  • 3 magnetometers like MFS-05, MFS-06e or MFS-07e

  • 3 magnetometer cables

  • 4 electric field probes

  • 4 electric field cables

  • 1 grounding rod + cable

  • Field computer (temporarily - may be any ruggedized laptop)


Typical 5-channel MT field setup

Connection of the Sensors to the ADU-07e

Now you can install the sensors:

  1. Dig the four EFP-06 into the soil and connect them with the input of the E-Field cable drum.

  2. Connect the other end of the 50m E-cable with the appropriate input terminals of the ADU-07e. The North-probe will be connected with the terminal labelled “N” of the ADU-07e. In the same way the “S”, “E”, “W” input terminals of the ADB are connected with the corresponding probes. Make sure that the E-Field cables are unreeled completely and the cable is not moving in the wind.

  3. Stick-in the delivered grounding rod close to the ADU-07e and connect it with the black GND-input clamp of the ADU-07e.

  4. Connect one end of the magnetometer cables with the HX, HY resp. HZ magnetometer. For this purpose first remove the magnetome­ter’s protection cap. Now push the end of the cable through the rubber flap in the middle of the protection cap. After having it connected with the socket properly, the magnetometer’s protection cap is pushed over the magnetometer’s head again. Please note that the reel of the magne­tometer cable (if there is one) always should be placed near the ADU-07e. The exact positioning and installation procedure of the magnetometer is de­scribed below. It is very important to notice the hints given there in order to obtain best results.

  5. Connect the plugs on the other end of the magnetometer cables with the corresponding input sockets on the ADU-07e i.e. the cable of the HX sensor with the socket labelled “HX”, the cable of the HY sensor with the “HY” socket and the cable of the HZ sensor with the “HZ” socket of the ADU-07e.

The correct direction of the sensors can be fixed by using a compass and two sticks:

A field helper rams the first stick into the soil according to the command of the other helper with the compass. The second stick is rammed behind the first stick. The correct alignment is found when the needle of the compass points to North for HX resp. East for HY and the sticks as well as the ring and bead sights of the compass are in line.

The horizontal direction is balanced using a level. The exact vertical position of the HZ-magnetometer can also be fixed by a level.

The magnetometers must be installed in a way that any movement of the sensors due to micro-vibrations is avoided. Such motion of an induction coil magnetometer in the stationary earth magnetic field would cause significant artificial noise. For this reason the hori­zontal magnetometers must be dug and covered by soil completely. The vertical HZ-com­ponent should be dug-in to at least half of its length or better to 4/5 of its length. An addi­tional coverage of the HZ sensor by a plastic bucket helps to reduce wind influences.


The cables close to the magnetometers must be fixed in a way that they cannot move in the wind!

Pinout of Connector Socket

Pin-out of magnetometer socket

Socket 10-pole ODU MiniSnap G32KON-T10QJ00-000 Pin









Sensor GND


Cal Signal+


Cal Signal -


Input +


Input -


\(I^{2}C\) SDA


\(I^{2}C\) SCL

The picture below shows the front side of the socket or the rear side of the corresponding plug with the solder cups.


You can order a suitable cable plug from Metronix or directly from the manufacturer ODU in Germany (

The part number of the plug is ODU Minisnap Series K S22KON-T10MJG0-7000

You may also need a strain relief streeve ODU 702023205965060

Wiring list of magnetometer cable MFS-06e/07e to ADU-07e

Target ODU MiniSnap Series K 10 pole

Origin ODU MiniSnap Series K 10 pole








\ twist





/ ed





\ twist





/ ed





\ twist





/ ed



Signal out


\ twist



Signal Return


/ ed





\ twist





/ ed




Trouble Shooting

This chapter describes our experience to localise possible errors of the system and methods how to fix them or get around it.

Parallel Sensor Test

In order to check the functionality of the sensors it is a good idea to perform a so called parallel sensor test. For this purpose 2 or more magnetometers are positioned horizontally and parallel with a distance of about 2 m from each other. Dig in the magnetometers. The electric field lines are laid out in parallel and perpendicular to the magnetic sensors. Use a single probe for each line (all together four of them). Now you record time series. If everything works fine you must see well correlated time series of the electric and the magnetic channels. A noisy sensor can be found out by this method easily.

Check of Magnetometer Cable

The pin-out of the magnetometer cable is given in chapter 0. Check the cable by using an Ohm-meter pin by pin according to the table. Also check for damages of the cable´s isolation.


Never pull the sensor out of the soil on its cable because either the cable connector or the sensor socket will be damaged by this procedure.

In Situ Measurement of Transfer Function

Metronix provides a software tool which allows to check the sensor´s transfer function in the field. This is achieved by a special joblist running on the ADU-07e which records some data for about half an hour. In course of this procedure test signals are fed into the calibration coil of the magnetometer. The software reads and processes the data and delivers the transfer function of the sensor as a result. You will find the necessary software on the USB key delivered along with the ADU-07e (you find it in the subfolder software).