
Hi all,
Many people are fooled by the difference between a square wave pulsed VLF and a PI detector. The truth is that an on-off square wave is just as usable in a VLF detector as is a sinusoidal transmit signal.
A square pulse contains energy at it's fundamental frequency as well as at harmonic frequencies. This is used to advantage in multi-frequency detectors.
Some advanced pulsed VLF detectors use a series of long and short pulses to provide the equivalent of transmitting a plurality of frequencies. All of these VLF detectors sample at least twice during each transmit cycle A first sample is taken from the receive signal at close to zero degrees and a second at ninety degrees relative to the phase of the transmit signal. Most multi-frequency detectors sample the receive signal twice for each frequency.
Each type of target provides an output signal from the demodulators which changes with different transmit frequencies. Multi-frequency detectors can thus make a finger print so to speak for each type of target as they collect more target information than single frequency detectors.
A single frequency VLF measures the ratio of the two demodulated signals. The ratio of these signals is often output as a number and is displayed as a target ID. Measuring the ratio of the two demodulated signals also provides the detector with it's discrimination ability.
A Pulse Induction detector is different from a VLF in as much as it transmits a signal by switching the battery voltage directly across the transmit or transmit - receive coil depending if the detector is using a balanced coil such as dual D or a simple mono coil.
Switching the coil across the power supply circuit causes a very heavy current to flow through it. the current causes a magnetic field to form around the coil. After a specific time period the coil is switched out of the circuit. A further short delay is provided so the circuit can settle down before one or more samples of the receive signal are taken. These samples are taken after the PI's transmit period ends unlike the VLF which samples during it's transmit cycles or pulses.
OK, back to the VLF. A VLF measures two components of the receive signal. The first component is in phase with the transmit signal and is due to the reactive component of the signal. This is referred to as "X" The second component is 90 degrees from the transmit signal and is due to the resistive component of the signal. This is referred to as "R". The mix or ratio of the "X" to the "R" component is what a VLF measures in order to discriminate. As the ground signal is almost a pure reactive signal then one can use the resistive component for a ground cancelling mode. A control or automatic circuit sets the "R" demodulator for a precise zero ground content. The clean "R" signal is an all metal signal.
The reactive or "X" component is required if we are to discriminate and or identify the target with a TID. The problem is that the ground signal adds and subtracts from the reactive signal as the coil moves across the ground which makes measurements useless. This problem has been solved to a certain degree in motion detectors by filtering both the reactive and the resistive signals with filters which are designed not to pass the slowly changing ground signal. Such filtering is employed prior to measuring the ratio of the signals. Both channels are filtered even though most if not all of the ground signal resides in the "X" component. This keeps the two signals together in their timing prior to their ratiometric comparison.
It is possible to make a hybrid VLF-PI. Such detectors are referred to as PIB's or Pulse Induction Balance detectors. The sample taken after the transmit pulse ends provides the "R" sample. a sample is also taken during the time that the transmitter coil is energized. This sample provides the "X" sample. A balanced coil is required for a PIB to discriminate. The coil can be either a dual D or a concentric coplanar. A balanced coil is required as the "X" sample is taken during the period when the transmit coil is energized.
In air any target can easily be discriminated using the "X" and "R" samples. Filtering is possible as with a VLF motion detector although depth is easily lost as the "X" sample is a little different from that which is obtained by a VLF. New methods and circuitry have recently overcome this problem 100%.
There is a bright future for PIB's. The marriage of the PI's depth capability and it's ability to ignore black sand etc. with the full range discrimination abilities of a VLF will provide super depth detectors with disc, notch, TID and all the features once thought reserved for the VLF detector with it's inferior depth capability.
I hope that this helps clear things up, Dave. * * *