ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING A simple metal detector with a piezo filter. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / metal detectors Purpose and opportunities This metal detector, despite the small number of parts and ease of manufacture, has a fairly high sensitivity. It can detect large metal objects, such as a radiator, at a distance of up to 60 cm, while small ones, for example, a coin with a diameter of 25 mm, can be detected at a distance of 15 cm. Operating principle The principle of operation of the device is based on the change in frequency in the measuring generator under the influence of nearby metals and the separation of the difference frequency (beats) between the measuring and exemplary generator. Since this frequency is in the audio range, it can be heard through headphones. Schematic diagram Schematic diagram of the metal detector is shown in fig. 2.46. In this circuit, the frequency of the reference oscillator, made on DD1.1, is stabilized using a piezoelectric element. A piezo filter (ZQ1) for an intermediate frequency (465 kHz), which is available in any household superheterodyne radio receiver, was used as a piezoelectric element. Such elements are widespread and much cheaper than quartz resonators. The use of a piezoelectric element makes it possible to increase the frequency stability of the reference oscillator compared to conventional LC or RC oscillators, and, therefore, increase the detection range of metal objects.
The measuring generator is assembled on a logic element DD1.2 and contains a coil (L1) in the form of a frame, which is a sensor. When the coil approaches the metal, its inductance changes, which leads to a change in the frequency of the oscillator. The initial frequency of the oscillator is determined by the elements C1C2C3L1 and is adjusted using an adjustable capacitor C1, close to the frequency of the reference oscillator (slightly more or less than 465 kHz). On the element DD1.3, the signals of the two generators are mixed. The output signal DD1.3 contains a difference harmonic, and in order to separate it from high-frequency pulses, a filter R3C5 is installed. The low-frequency signal is amplified by the field-effect transistor VT2 and fed to the sound emitter - headphones BF1 BF2. The use of CMOS microcircuits in self-oscillators, due to their large input resistance, makes it possible to obtain a high quality factor in the oscillatory circuit of the search oscillator, which increases its frequency stability. This makes it possible to work with small beats and thus increase the sensitivity of the metal detector. The power supply of the autogenerators is stabilized using a precision KS166V zener diode. Only parametric stabilizers for a voltage of about 6 V have a voltage drift close to zero with a change in ambient temperature. The metal detector circuit remains operational when the voltage drops to 5 V, but in this case there will be no stabilization of the supply voltage. The current consumed by the metal detector (and, therefore, the duration of operation) is highly dependent on the resistance of the headphones connected at the output. For this reason, their resistance should be as high as possible (> 100 ohms), for which the phones in the headphones are connected in series. Resistor R7 limits the maximum current of the transistor VT2 in case of a short circuit in the headphones, and resistor R6 allows you to adjust the sound volume. For convenience, this resistor is combined with the SA1 power switch. Headphones are connected through any standard socket. Socket X2 is designed to connect a mains charger for the G1 battery. This will allow you to recharge the batteries without removing them from the case. Element base Tuning capacitor C1 can be taken from any miniature radio receiver (for example, KP-180). C2 and C3 must be with a minimum negative TKE (M47, M75), C4 and C5 from the K10 series (K10-17), C6 - K53-1 at 16 V. The variable resistor R6 is SP3-3bM (it provides for horizontal installation on the board and has a built-in SA1 switch), a tuned resistor R5 of the SPZ-19a type, the rest will fit any small ones. A piezo resonator (piezo filter Z01) is likely to fit any of the FP1P1-61 series (-01, -02, etc.), and you can also try many other types of piezo filters from Chinese receivers that have three outputs. Printed circuit board The details of the device can be located on a single-sided printed circuit board made of fiberglass with a thickness of 1,5 mm and dimensions of 75 x 40 mm (Fig. 2.47, a-b). It is desirable to place the board near the sensor coil L1. The place where the board with the elements is fixed does not need to be shielded. Coil making The metal detector sensor coil L1 has the form of a toroidal frame, (Fig. 2.47, c). It is wound with a copper wire PEV with a diameter of 1,2 mm, on any suitable mandrel with a diameter of 20 cm, for example, cut out of foam. Winding should be carried out in bulk, 30 turns (the inductance is about 480 μH). After winding the coil, the frame must be wrapped with any dielectric tape (varnished cloth or electrical tape), and then with thin aluminum foil. You can also use copper foil. At the place of the coil leads, a section of about 10 mm should not be covered with foil (a gap is left between the ends of the screen, as shown in Fig. 2.47, c).
The screen at the coil reduces the influence of parasitic capacitances, which increases the stability of the operating frequency of the search oscillator. The use of thick wire in the manufacture of L1 provides a higher quality factor for the coil and stiffens the frame without the use of additional fasteners. Author: Shelestov I. See other articles Section metal detectors. Read and write useful comments on this article. Latest news of science and technology, new electronics: Artificial leather for touch emulation
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