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Instruments
A measurement of the magnetic field at any location will
involve either recording the magnitude in one or more vectorial
coordinate directions, or a magnitude in the field's direction
(commonly referred to as "total field strength"). There are many
manufacturers of magnetometers for ground, marine, helicopter, fixed
wing, and space-borne geophysical use. Instrument types commonly used
are outlined very briefly as follows:
Fluxgate Magnetometer
- This type of instrument was developed during WWII to detect
submarines. It measures the magnitude in a specific direction
determined by the sensor's orientation. A complete measurement of the
field requires three individual (cartesian) components of the field (
such as Bx,
By, Bz).
- It is generally difficult to get leveling and alignment
accurate. Sensor accuracy is 1 nT so orientation must be known to
within .001 degrees.
- There are some fluxgates which generate a measure of the total field strength.
Proton Precession Magnetometer
- This instrument was the most common type before the mid 1990's. It measures
the total field strength.
- Advantages: Sensitive to 1 nT, small, rugged & reliable, not sensitive to orientation.
- Disadvantages: Takes >1 sec to read, sensitive to high gradients.
- The measurement process is related to nuclear magnetic resonance (NMR).
A proton source (possibly as simple as a volume of water) is subjected to an artificial
magnetic field, causing the protons to align with the new field. When the artificial
field is removed, the protons precess back to their original orientation and
their precession frequency (called the Larmor precession frequency) is measured. That frequency, f,
is related directly to the strength of the earth's field according to the
equation to the right. The parameter, p,
is the ratio of the magnetic moment to spin angular momentum. It is
called the gyromagnetic ratio of a proton and is known to 0.001%; p = 2.67520 x 108 T-1s-1.
Cesium (or optically pumped) magnetometer:
- The physics behind this
type of sensor is related to that of the proton precession sensor, but it
is more complicated. Although it is more expensive than the above two sensor
types, it is now the most commonly used system for small scale work because
it is 10 to 100 times more sensitive than the proton precession magnetometer.
- The measurement process makes use of the gyromagnetic ratio
of electrons and of the quantum behavior of outer-shell electrons of
some elements (e.g. cesium). In this case, the relevant gyromagnetic
ratio is known to 1 part in 107 , and frequencies are near 233 khz, so these instruments are sensitive to 0.01 nT.
- Advantages: More rapid readings, 1 or 2 orders of magnitude more sensitive, works in high gradients.
- Disadvantages: Optical pumping won't work when parallel or
perpendicular to mag field direction (solved with multiple sensors),
more expensive than proton precession.
SQUIDS (superconducting quantum interference devices): These are
very sensitive, and are currently more common in laboratories that work on
rock magnetism or paleomagnetic studies. However, they are beginning to be
used in the field, and more applications will become evident in the coming
decade (2000 - 2010). Search the internet using, for example, "squid AND
magnetometer AND geophysics" as keywords.
Magnetic Gradiometer
- These instruments use two sensors (any of those mentioned above) to measure vertical or horizontal gradients.
- They often employ two cesium magnetometers separated by about 1 m.
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