# A Current Sensing Cross-Component Induction Magnetometer for Use in Time-Domain Borehole Geophysical Electromagnetic Surveys

**Authors:** Joseph Hamad, James Macnae

PMC · DOI: 10.3390/s25061646 · Sensors (Basel, Switzerland) · 2025-03-07

## TL;DR

This paper introduces a new current-sensing magnetometer for borehole geophysical surveys that improves sensitivity and bandwidth over existing methods.

## Contribution

A novel cross-component induction magnetometer (CCIM) using current sensing instead of voltage for improved performance in borehole TEM.

## Key findings

- The CCIM achieved a low-cut corner frequency of 3.5 Hz with noise levels comparable to fluxgate magnetometers at higher frequencies.
- The CCIM outperformed fluxgates above 10 Hz with noise levels as low as 0.1 pT/√Hz.
- Induction coils for cross-components offer high-frequency bandwidth and compatibility with fluxgate sensors in downhole packages.

## Abstract

Electromagnetic sensors are best defined by their linearity, signal sensitivity, and noise level. In borehole time-domain electromagnetics (TEM) the cross-components are defined as the two components perpendicular to the borehole’s axial direction. Induction sensors measuring voltage across an open coil for the cross-components have poor sensitivity, and fluxgate magnetometers have been a common band-limited alternative for borehole TEM surveys. In this research, we use a shorted coil with current rather than voltage sensing circuitry to produce a cross-component induction magnetometer (CCIM). With flux coupling and electronic adjustments, we achieved a low-cut corner frequency of 3.5 Hz in the final design of the CCIM. For the prototype sensor, we found the simple ratio of measured inductance L to winding resistance R to be a poor predictor of the −3 dB corner frequency, and a transfer function measurement was required. The cause of the discrepancy may be that the self-inductance measured by a meter is different from the coupling inductance to an external field. The measured noise level of our CCIM sensors was 125 pT/√Hz at 1 Hz, compared to a geometrically longer axial component sensor with 4 pT/√Hz at this frequency. However, our design matched the typical fluxgate noise level of 6 pT/√Hz at 10 Hz. Further, the CCIM sensors were superior to fluxgates at frequencies higher than 10 Hz, with an internal noise level of 0.1 pT/√Hz between 100 Hz and >20 kHz. Induction coils or magnetometers measuring the cross-component are attractive because they have excellent high-frequency bandwidth and can be included in the same downhole package with fluxgate sensors.

## Full-text entities

- **Diseases:** injury to (MESH:D014947)
- **Chemicals:** 2714A foil (-), nickel sulfides (MESH:C017558), copper (MESH:D003300), Ferrite (MESH:C001215), carbon (MESH:D002244), nickel (MESH:D009532)
- **Species:** Homo sapiens (human, species) [taxon 9606]

## Full text

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## Figures

13 figures with captions in the complete paper: https://tomesphere.com/paper/PMC11945872/full.md

## References

44 references — full list in the complete paper: https://tomesphere.com/paper/PMC11945872/full.md

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Source: https://tomesphere.com/paper/PMC11945872