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NUMIS
Plus
Proton Magnetic Resonance System
Features
The NUMISPlus
system allows the direct detection of groundwater through measurements of
the relaxation magnefic field produced by Hydrogen protons from
groundwater after they were energized by a current into a loop laid on the
ground. It is a modular and more powerful version of the original NUMIS
system.
NUMISPlus equipment consists of
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two converter units powered by two 12 V batteries,
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two tuning units for optimizing the excitation energy,
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a transmitter-receiver unit for pulse generation and signal
measurement, a wire loop used both as a transmitting and a receiving
antenna,
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a PC computer for the control of the whole system, and for data
processing and interpretation.
AQUIFER PARAMETER EVALUATION
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NUMISPlus schematic diagram |
PMR FOR
GROUNDWATER
The field application of the Proton Magnetic Resonance (PMR) method is
based on a well established theory. PMR is the only non-invasive method
which directly studies groundwater reservoirs from surface measurements.
PRINCIPLE OF THE METHOD
Hydrogen atoms of water molecules are energized by pulses of
alternative current at the proper frequency (Larmor frequency),
transmitted into a loop laid on the ground. The magneto field they produce
in return is measured and analyzed for various energizing pulse moments
(intensity x duration).
INFORMATION OBTAINED
The interpretation of measurements permits to estimate the water
content and the mean pore size of each layer at depth. These parameters
are useful to determine the prospects of a groundwater reservoir before
drilling.
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The static field B, (Earth’s magnetic field) determines the Larmor
frequency of the H protons: F(Hz) = 0.04258' Bo (nT)
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The dynamic energizing field B, (loop magnetic field) produces the
nutation of the H protons magnetic moment M, @ it @its away from the
static field with an angle 0, while still processing at ft Larmor
frequency.
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Once the energizing field has been switched off, the protons come
back to equilibrium (Mo aligned with Bo) after a relaxation dewy
characterized by an initial amplitude Eo, and a time constant T2*.
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The water content is proportional to the amplitude of the proton
response.
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The pore size of the medium (which is linked to the permeability)
determines the time constant of this dewy response.
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The depth of investigation is determined by the intensity of the
energizing pulse.
PMR FIELD MEASUREMENTS
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The transmitting antenna consists of a 150 m wide square loop laid
on the ground, allowing a depth of investigation of the order of 150
m.
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The Larmor frequency varies between 0.8 and 3.0 kHz depending on the
amplitude of the local Earth’s magnetic field.
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The energizing current in the loop will reach intensities of 300 -
450 A during pulses of a few tens milliseconds.
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The relaxation field of the protons is measured in the same loop,
after the energizing current is turned off.
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The voltage measured in the loop is in the order of a few tens to a
few thou- sands nanovolts. Stacking is used to enhance the signal.
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Taking the readings corresponding to a complete PMR sounding with a
full set of pulse moments, usually takes less than one hour per
station.
NUMIS
DATA ACQUISITION SOFTWARE
During the acquisition the operator monitors on the PC screen the
signal curve (the envelop of the proton response, an exponential decay
curve), and a noise curve stacked in the same conditions as the signal
curve.
The number of stacks to use depends on the signal/noise ratio and has
to be set by the operator according to the local noise level. In case of
high noise conditions, an eight-shape loop can be used to significantly
improve the quality of the measurements, although it reduces the
investigation depth.
INTERPRETATION OF PMR DATA
The PMR theory states that the investigation depth of a measurement
varies with the moment of the excitation pulse (product of the intensity
of current at the resonance frequency by the duration of the pulse). It is
therefore possible to sound the ground with PMR surface measurements.
Besides, it can be shown that the decay time constant of the relaxation
field is related to the pore size, which potentially.permits to
distinguish between pore free water and clay bound water.
For interpreting a PMR sounding, it is assumed that the underground is
stratified at the scale of the loop dimensions. The inversion gives
estimates of the water content, the mean pore size and the depth of each
layer, after processing of the raw data for the whole set of pulse
moments. For inverting a set of field data it is first necessary to
compute a matrix giving the theoretical response of thin water layers
located at various depths. This matrix will take into account the general
configuration of the measurements: loop dimension, Earth’s field
inclination, ground resistivity, ... The computation of this matrix may
take several hours on a PC but the results will be valid for all the
soundings of a given survey, Then the inversion itself of one set of data
will take only a few seconds: the results can thus be available in the
field before moving the equipment to the next site. The inversion
procedure is fully automatic: no initial model is required. The operator
has the possibility to manually change the value of the regularization
parameter for smoothing or enhancing the variations of the water content
with depth according to the local context (equivalence properties).
PMR VERSUS OTHER GEOPHYSICAL METHODS
PMR is a direct method for groundwater detection, as it directly
measures the response of the water itself (H protons). The more
traditional methods (DC, TDEM, ..), are indirect ones, as they measure a
physical parameter which is only indirectly linked to the presence and to
the quantity of water: the electrical resistivity of the layers is a
function not only of the porosity (volume of water) but also of the
resistivity of the water; besides, the formation resistivity is also
influenced by the conductivity of clay which makes the interpretation
sometimes complex.
In terms of depth determination, PMR is influenced, as other
geophysical methods, by equivalence rules, due to the fact that it is an
integrating method. However, for PMR, the eigen parameter is the product
of the water content by the thickness of the layer, which means that the
total quantity of water is always fairly well determined.
A particularity of PMR is the non linear relationship between the
measured signal and the energizing pulse intensity. This means that
doubling the pulse current does not mean doubling the signal: instead it
increases the depth of investigation. On the other hand, the PMR signal is
linearly related to the water content of the layers, which makes the
interpretation quite quick.

NUMISPLUS MAIN FEATURES
NUMISPLUS is a modular equipment designed to
allow measurements at remote locations, as each component of the system
weighs 25 kg or less, making it one man portable. The Tx/Rx unit is the
core of the system. It ensures the production of the energizing pulses at
the Larmor frequency, also the measurement of the PMR response with
filtering, amplification and analog to digital conversion. The PC computer
receives raw data, then process, display and store them for further
interpretation. The two DC/DC converter units are required for a maximum
investigation depth of 150 m), to energize the 150 m side square loop (600
m total length). However, if an investigation of 100 m is sufficient one
converter unit only is required with a I 00 m side square loop (400 m
total length) The two tuning units must be used at lower magnetic
latitudes (for an Earth’s field lower than 31 000 nT with the 150 m side
square loop, or 37 000 nT with the 100 m side square loop), while one
tuning unit only is needed at medium and higher latitudes.
NUMISPLUS
TECHNICAL SPECIFICATIONS
DC/DC CONVERTER UNIT
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Power supply: two 12 V batteries (60 Ah each)
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6 to 8 hours reading autonomy
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Capacitance: 0.05F
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Outputs: d: 400 V DC ; 0. 5 A
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Two converters may be used in parallel.
TRANSMITTER SPECIFICATIONS
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Supplied by one or two DC/DC converters
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Frequency range: 0.8 to 3 kHz
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Maximum outputs: 4000 V, 450 A
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Pulse amplitude and duration: programmable
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Pulse moment: 100 to 18000 A.ms (loop and frequency dependent)
RECEIVER SPECIFICATIONS
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Band pass filter width: 100 Hz
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Programmable gain: 104 to 106
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Noise: less than 10 nV / sqrt(Hz)
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AID converter: 14 bits
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Sampling frequency: four times the Larmor frequency
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Calibration procedure for phase reference
TUNING UNIT
TRANSMITTING / RECEIVING LOOP
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Reels of 100 m wire, 10 mm2 section
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Six reels for 150 m investigation: impedance 1.0 ohm, 1.1 mH
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Four reels for 100 m investigation: impedance 0.6 ohm, 0.7 mH
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Other loop configuration on request
PC COMPUTER
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Control of the whole system: converter, transmitter, receiver
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Data processing: DFT and weighted stacking
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Data interpretation: 1D inversion
Ordering Information
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Description
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Order Number
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NUMIS plus
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175-850-0211b
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