Metal Detection: Prospecting With A Hoover
Metal Detection: Prospecting With A Hoover
BY THE PROF
Although the “treasure” hunting craze of the seventies seems characteristics of the coil that a piece of metal in reasonably
to have waned considerably during the eighties, metal detection close proximity is likely to have. However, some detectors have
still remains a popular aspect of electronics. It is also one that, coils which detect changes in a radiated signal, rather than
perhaps after some over-kill in the past, has received very little directly detecting the metal. As far as I can ascertain, all normal
attention in the technical press over the last few years. Even if forms of metal detector use a search coil of some sort or other.
you are not interested in going out into the wilds in search of
In this article I will provide basic details of all the types of
Practical Electronics July 1988 - Copyright Wimbourne Publishing
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A high operating frequency and the heterodyne principle are used in practice though. A very simple method that I have
used to give improved sensitivity. The output from the search found to be quite effective is to have an oscillator which
oscillator and a second oscillator are fed to a detector and rf includes the search coil in its L-C tuned circuit, and to also
filter. The output from the filter is the “beat” note, which is have an accurate voltage monitoring circuit of some type
merely the difference between the frequencies of the two included in the unit. When metal is brought near to the coil it
oscillators. These are tuned so that the beat note is a low audio produces a change in the operating frequency, but probably of
frequency. If, for example, the search oscillator operates at greater importance in this case, it alters the 0 value of the coil.
199kHz and a metal object produces. a 0.01% reduction in The voltages in an oscillator are not exclusively under the
frequency in absolute terms this represents a shift of 10Hz. This control of the bias network, and in many cases the bias circuit
is not very much, but if the beat note was set at 50Hz, this exerts very little control. The change in 0 and operating
would give a 20% reduction in output frequency, with an actual frequency will give small voltage shifts with many oscillator
output frequency of 40Hz. This would be clearly detectable by designs, and these can be detected by the voltage monitoring
the human hearing mechanism. By contrast, direct operation at circuit.
50Hz and a 0.01% shift in frequency would given an inaudible
Vast numbers of metal locators must have been manufactured
shift of just 0.005Hz!
over the last ten to fifteen years, and one might reasonably
SENSITIVITY expect that there would be several special integrated circuits for
this purpose. This does not seem to be the case though, and the
For optimum sensitivity a high search oscillator frequency
commercial detectors I have seen have had circuits based on
Practical Electronics July 1988 - Copyright Wimbourne Publishing
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generally much clearer than the varying tone produced by a bfo
detector.
The output from the amplifier is fed to a detector circuit that
gives a dc output level which is proportional to the output level
from the amplifier. If meter indication is required, the meter can
be driven from the detector stage via a buffer amplifier. For an
audio output the next stage is a dc amplifier which incorporates
a shift control that can be used to raise the quiescent output
voltage above its normal level of close to zero. In practice this
control sets the volume of the output tone under stand-by
conditions, and results are generally better with a quiet tone
rather than having zero output under quiescent conditions. This
control is sometimes (rather confusingly) referred to as a
that the oscillator can not cease oscillating even if a very large
“tuning” control incidentally.
piece of metal is placed close to the search coil.
The next stage is a “chopper”, which is merely an electronic
For those who would like to experiment with the CS209 the
switch that gates the output of the dc amplifier on and off. This
basic metal detector circuit of Fig. 3 is provided. The data sheet
generates a squarewave signal having a peak to peak amplitude
for this device recommends a value of about l00µH for L1, but
Practical Electronics July 1988 - Copyright Wimbourne Publishing
We have the familiar oscillator and search coil, but this time
with a second coil feeding into an amplifier. Although a strong
coupling from the coil driven by oscillator to the second coil
would be expected, careful positioning of the two coils provides
what is a very inefficient coupling with no significant output This type of detector operates in what is essentially the same
from the pickup coil. This sounds difficult, but is achieved manner as the two coil ib type, with metal in the vicinity of the
merely by partially overlapping the two coils. A piece of metalsearch coil upsetting the balance of the system, and producing a
close to the coils produces an imbalance and gives a strong stronger output from the amplifier. With both types it seems to
output from the amplifier stage. be normal to have the system adjusted so that under quiescent
conditions there is considerably less than perfect balancing.
There must be endless ways of converting this rise in signal
This enables the unit to discriminate between ferrous and non-
level into some form of indication to the operator of the
ferrous metals. The latter give a decrease in coupling whereas
equipment, but the general method shown here seems to be a
the former produce increased coupling.
popular one. It provides an audio output tone that rises in
volume when metal is detected. This form of indication is
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Many of the more up-market ib designs have quite potentiometer so that the signal level can be adjusted for precise
sophisticated discrimination capabilities. This generally takes cancelling. As for the ib type, metal close to the search head
the form of a control that enables the unit to be nulled on a alters the strength of the signal from the pick-up coil, giving an
piece of metal, and it will then fail to respond (or at least be imbalance in the signal levels fed to the mixer and producing an
very insensitive to) any pieces of that particular metal in the output from the mixer. This signal is fed to a detector stage, and
search area. A typical use of the discrimination facility is to the resultant dc signal is amplified before being applied to a
render the detector insensitive to aluminium foil, which is meter. Of course, the dc signal can be fed to a chopper and
found in large quantities in many popular types of hunting audio amplifier if an audio indication is required as well. As the
ground. Note that discrimination means the ability of a detector t/r type of detector operates on what is really the same principle
to ignore certain metals: it does not mean the ability to ignore as the ib type, it has very much the same advantages and
everything but (say) gold or silver. In my experience the drawbacks.
discrimination facilities of metal detectors are less worthwhile
OFF-RESONANCE
than much of the advertising literature would have you believe.
There is often a penalty to pay in the form of reduced This seems to be a little used type of detector, and it utilises
sensitivity, and setting up a machine which has adjustable the setup shown in Fig.7. It is another type of detector that
discrimination and other advanced features can make setting up relies on a balancing process, but the operating principle is not
a video recorder to automatically record a programme look like the same as the ib and t/r types. In fact it is much more like the
child’s play. bfo type of detector in this respect.
Practical Electronics July 1988 - Copyright Wimbourne Publishing
PULSE TYPE
Pulse induction detectors operate on a principle that is
completely different to ib and bfo style detectors. Fig. 8 shows
a somewhat simplified block diagram for a pulse induction
detector.
The principle of operation may be different, but a search coil
is still central to the operation of the system. A pulse generator
supplies brief pulses to the coil, and this generates a magnetic
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up that drives an amplifier. Note that the coils are not arranged
field around the coil. On the trailing edge of each pulse the in such a way as to give zero output from the pick-up coil.
magnetic field collapses and generates a reverse voltage across Operation of this system relies on a reasonably strong output
the coil. The coil must be damped (electrically that is!) so that signal being obtained from the pick-up coil. The output signal
the reverse voltage spike decays quite rapidly. If there is a piece of the oscillator and the output of the amplifier are fed to
of metal in the vicinity of the coil it will either produce an eddy squaring circuits, as shown in the block diagram of Fig. 9.
current or become magnetised by the field of the coil,
depending on whether the metal is non-ferrous or ferrous. As The effect of metal close to the search head is to produce a
far as the effect on the reverse pulse from the coil is concerned, phase shift in the output from the pick-up coil. Linear or digital
in either case the pulse becomes stretched. circuits could be used to detect this phase change and convert it
Practical Electronics July 1988 - Copyright Wimbourne Publishing