Low temperature squid transient electromagnetic receiver system

CA 02600567 2007-09-10

WO 2006/095251

PCT/IB2006/000509

-1LOW TEMPERATURE SQUID TRANSIENT ELECTROMAGNETIC RECEIVER SYSTEM

BACKGROUND OF THE INVENTION

THIS invention relates to a transient electromagnetic receiver system, and to a method of collecting data in an electromagnetic prospecting system.

Typical prospecting systems comprise a transmitter for transmitting a primary electromagnetic field into the ground. A receiver, comprising either a one-component or a three-component receiving coil and associated electronics, is provided for receiving and recording a resulting, secondary electromagnetic field produced by eddy currents emanating from the interaction between underground ore bodies and the primary electromagnetic field. Generally, insignificant eddy-current induced secondary electromagnetic fields are received in areas where the ground has an average to low electrical conductivity, whereas in more conductive areas stronger eddy currents tend to be generated, thereby causing an appreciable secondary electromagnetic field to be created.

The secondary electromagnetic field is a transient field having a decaying profile 10 of the type shown in Figure 1, wherein the y-axis is the secondary field amplitude, on a log scale, and the x-axis is time, on a log scale. Typically, the receiving coil of the receiver comprises three orthogonal sensors, which detects the secondary field in the range indicated by arrow

12. It is clear from arrow 12 that the highest detection level of the receiver is set to just above the maximum value of profile 10, with the lowest level of the receiver defining a threshold 14, due to the physical limitations of the receiver. It is thus clear from Figure 1 that the secondary field after time L, corresponding to broken line component 16 of the response, would not be detected.

CONFIRMATION COPY

CA 02600567 2007-09-10

WO 2006/095251

PCT/IB2006/000509

-2It would, however, be desirable and useful to detect the secondary electromagnetic field after time ti in addition to the field response before time fi. This may, for example, indicate the presence of conductive ore bodies located relatively deeper underground. The present invention is aimed at addressing this shortcoming of existing electromagnetic prospecting systems and methods.

SUMMARY OF THE INVENTION

According to a first aspect of the invention there is provided an electromagnetic prospecting system comprising:

a transmitter for transmitting a primary electromagnetic field so as to generate a secondary electromagnetic field from a terrain that is being prospected, the secondary electromagnetic field having a transient, decaying time domain profile; and a receiver system comprising first and second sensors for detecting the secondary electromagnetic field, wherein the second sensor is less sensitive than the first sensor so as to detect the secondary electromagnetic field over a first time period, with the first sensor being used to detect the secondary electromagnetic field after the first time period.

Conveniently, the electromagnetic prospecting system further includes a data collector that is connected to the first and second sensors, for collecting and recording field data over the entire decay curve of the secondary electromagnetic field.

Preferably, the data collector collects and records field data over the entire decay curve of the secondary electromagnetic field to a lower sensitivity level of 5 fT/λ/Ηζ for subsequent processing.

CA 02600567 2007-09-10

WO 2006/095251

PCT/IB2006/000509

-3ln an example embodiment, the second sensor is approximately 10 times less sensitive than the first sensor.

Typically, each sensor comprises three orthogonal magnetometers.

Conveniently, the magnetometers of the first and second sensors are low temperature superconducting quantum interference device (SQUID) magnetometers.

According to a second aspect of the invention there is provided a receiver system for an electromagnetic prospecting system comprising a transmitter for transmitting a primary electromagnetic field so as to generate a secondary electromagnetic field from a terrain that is being prospected, the secondary electromagnetic field having a transient, decaying time domain profile, the receiver system comprising first and second sensors for detecting the secondary electromagnetic field, wherein the second sensor is less sensitive than the first sensor so as to detect the secondary electromagnetic field over a first time period, with the first sensor being used to detect the secondary electromagnetic field after the first time period.

Conveniently, the receiver system further includes a data collector that is connected to the first and second sensors, for collecting and recording field data over the entire decay curve of the secondary electromagnetic field.

Preferably, the data collector collects and records field data over the entire decay curve of the secondary electromagnetic field to a lower sensitivity level of 5 fT/^Hz for subsequent processing.

In an example embodiment, the second sensor is approximately 10 times less sensitive than the first sensor.

Typically, each sensor comprises three orthogonal magnetometers.

CA 02600567 2007-09-10

WO 2006/095251

PCT/IB2006/000509

-4Conveniently, the magnetometers of the first and second sensors are low temperature superconducting quantum interference device (SQUID) magnetometers.

According to a third aspect of the invention there is provided a method of collecting data in an electromagnetic prospecting system comprising a transmitter for transmitting a primary electromagnetic field so as to generate a secondary electromagnetic field from a terrain that is being prospected, the secondary electromagnetic field having a transient, decaying time domain profile, the method comprising the steps of:

providing a receiver system comprising first and second sensors for detecting the secondary electromagnetic field, wherein the second sensor is less sensitive than the first sensor using the second sensor to detect the secondary electromagnetic field over a first time period; and using the first sensor to detect the secondary electromagnetic field after the first time period.

Typically, the method further includes collecting and recording field data detected by the first and second sensors over the entire decay curve of the secondary electromagnetic field.

Preferably, the method includes collecting and recording field data over the entire decay curve of the secondary electromagnetic field to a lower sensitivity level of 5 fTh/Hz for subsequent processing.

CA 02600567 2007-09-10

WO 2006/095251

PCT/IB2006/000509

-5BRIEF DESCRIPTION OF THE DRAWINGS

Figure 1 shows a typical transient response of a secondary electromagnetic field produced by deep ore bodies that have been excited by the transmission of a primary electromagnetic field into the ground; and

Figure 2 shows a schematic diagram of an electromagnetic prospecting system according to the present invention that allows recording of the secondary electromagnetic field both before time ti shown in Figure 1 and after time tv

DESCRIPTION OF THE PREFERRED EMBODIMENT

Referring to the figures, a receiver system 18 for use in an electromagnetic system according to the present invention comprises a first, relatively sensitive, sensor 20, and a second sensor 22 that is less sensitive than the first sensor 20. Typically, the second sensor 22 is 10 times less sensitive than the first sensor 20, so as to provide a larger dynamic and slew rate than the first sensor. Thus, the first sensor 20 is used to detect the secondary electromagnetic field after time fi, whereas the second sensor 14 is used to detect the field before time tv

Each sensor 20, 22 comprises three orthogonal magnetometers 24A, 24B and 24C, and 26A, 26B and 26C, respectively.

Preferably, the sensitivity of the second sensor is around 50 fTA/Hz, and the sensitivity of the first sensor is around 5 fTA/Hz, resulting in the second sensor having a 10 times higher slew rate. Thus, the first sensor 20 is designed to measure the late times of the time domain electromagnetic decay shown in Figure 1 with high precision, whereas the second sensor is designed to measure the early times of the decay. This enables the system

CA 02600567 2007-09-10

WO 2006/095251

PCT/IB2006/000509

-6to accurately measure the decay curve over the entire time span of the signal.

Both first and second sensors 20, 22 are low temperature superconducting quantum interference device (SQUID) magnetometers. The sensors will thus typically be encased within a liquid Helium-filled cryostat, although this is not shown in the diagrams in order to clarify the description of the invention. Significantly, the cryostat is specifically designed to have a minimum of metal parts that could interfere with TEM measurements, yet that has efficient temperature control characteristics to allow 24 hour helium refilling intervals.

The first and second sensors 12, 14 are connected via control, auto-tuning and amplifying electronics 28, to a data collector 30, for collecting and recording field data over the entire decay curve of the secondary electromagnetic field. The six inputs into the data collector 30 thus define a six-channel magnetometer SQUID system having characteristics suitable for high sensitivity TEM measurements.

The high- and low-sensitivity sensors can be switched on to operate separately as well as simultaneously via switches on the control electronics 28. Preferably, the control electronics 28 incorporates a circuit to determine the slew rate of the magnetic field by the data acquired by the second magnetometer 22 and controls the operation mode of the first sensor 20. By this means, the first magnetometer 20 is only operated if the slew rate is small enough to allow its stable operation.

Thus, referring back to Figure 1, the receiver of the present invention will not only be able to pick up the secondary field in the range indicated by arrow 12, but also in the range indicated by arrow 32.