ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Field strength meter. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Civil radio communications When establishing the equipment and antennas of an amateur radio station, it often becomes necessary to measure the level of electromagnetic radiation in the radio frequency range. Professional equipment for such measurements is rarely available to radio amateurs, but with an accuracy acceptable for practice, it is possible to estimate the electric field strength created by a radio station using simple home-made devices. Recently, considerable attention has been paid to measures to limit the effects of electromagnetic radiation on humans. These issues are regulated by federal sanitary rules, norms and hygienic standards [see, for example, 1]. In our country, for residential premises, the maximum permissible levels of electric field strength are 10 V / m (for a frequency band of 3 ... 30 MHz) and 3 V / m (30 ... 300 MHz). In a number of European countries, there are similar standards for electric field strength levels. If, by the way, they are not exceeded, then the communications administrations of the country do not accept claims against the transmitting radio station for interference with other electronic devices (for example, audio equipment). In particular, for the frequency band 30...300 MHz, this level is also set to 3 V/m [2]. In other words, if the electric field strength created by a radio transmitting device is considered safe for humans, then this level must also be "tolerated" by electronic household equipment. The foregoing implies that the owner of an amateur radio station must be prepared for controversial situations and be able to at least roughly assess the levels of electric field strength that his radio station creates in residential premises. In the VHF bands, these levels can be measured using a conventional half-wave dipole. As you know, the voltage U induced in the antenna is equal to its effective height multiplied by the electric field strength of the electromagnetic wave. For a half-wave dipole, the effective height is λ/π where λ is the wavelength [3]. In the amateur VHF band of 2 meters with a field strength of 1 V / m, the voltage U will be 0,66 V for an unloaded dipole and 0,33 V when loaded with a resistor with a resistance equal to the input resistance of the dipole (73 ohms). Such voltages can already be recorded with a conventional high-frequency voltmeter with a diode detector. The meter turns out to be simple and does not contain a power source. If a high-frequency voltmeter connected to a loaded dipole registers a voltage of 1 V (effective value), then the full-scale deviation of the meter needle will just correspond to an electric field strength of 3 V/m. "Scaling" of the indicator of the device will indicate that at this point the maximum allowable value of the field is exceeded The scheme of the electric field strength meter for the range of 2 meters is shown in the figure. The halves of the dipole are made of copper wire with a diameter of 2...3 mm. The dimensions in the figure are given in cm. The elements of the high-frequency voltmeter are placed on a small plate of insulating material, to which the halves of the dipole are also attached. The high frequency voltmeter uses a germanium diode because silicon diodes are not suitable for measuring low RF voltages. In addition to the GD508A diode indicated on the diagram, GD507A and D311 can be used here. For germanium diodes of other types (among the common ones), the detection efficiency at frequencies above 30 MHz is noticeably reduced. The values of resistors R1 and R2 are given for a measuring head with a total deflection current of 100 μA and a loop resistance of 2,85 kOhm (M4247). If the radio amateur has the opportunity to calibrate the high-frequency voltmeter (set the upper measurement limit by selecting resistors R1 and R2, and also remove the dependence of the voltmeter readings on the applied RF voltage), then upon completion of this procedure, the production of the field strength meter ends. Calibration can be done using a VK7-9 voltmeter or similar devices. When selecting resistors, it is useful to observe the condition R1 = R2 for better antenna symmetry. Of the design features of the device, only one should be noted. To reduce the influence on the measurements of the operator's body, and especially his hands, a small "mast" (not shorter than 0,5 m) must be attached to the antenna with an indicator and the entire structure should be held at arm's length. If the radio amateur does not have the opportunity to calibrate the RF voltmeter of the field strength meter, then you can use the method below. The total resistance of resistors R1 and R2 is chosen so that the DC voltmeter (these resistors and microammeter) has a voltage measurement limit of 1 V. Their resistance (in kOhm) can be calculated from the ratio R1 = R2 = (1/iR)/2, where i is the total deflection current of the RA1 device, mA; R is its internal resistance, kOhm. In this case, the RF voltmeter will also have a measurement limit close to 1 V (effective value), with an error of no more than 20%, regardless of the diodes used in the voltmeter (from among those mentioned above), and the scale of such an RF voltmeter will be a power law with an exponent degree n ~ 1,25. You can read more about this in [4]. For a microammeter with a total deflection current of 100 μA, the correspondence between the instrument readings N and the true values of the RF voltage U (effective value) is shown in the table. For microammeters with other values of the total deflection current, the exponent n changes (but not much, see [4]) The error in measuring the RF voltage with such an RF voltmeter (and, consequently, the electric field strength generated by the transmitter) will not exceed 30%, regardless of the diode instance used. The accuracy is not high, but it is quite sufficient for rough estimates of the electromagnetic environment. The structure of the electromagnetic field in residential premises can be very heterogeneous due to the reflections of radio waves from metal structures and electrical wiring. For this reason, the indicator must be moved near the measurement point, achieving the maximum of its readings, as well as varying its polarization. It is impossible to make a similar resonant field meter for lower frequencies due to the large length of the dipole, but for estimates in the KB ranges, the one described above can also be used using it as a Hertzian dipole (very short compared to the wavelength). The effective height of an unloaded Hertzian dipole is -l/2, where I is the total length of the dipole (in our case, about 1 m). Therefore, for example, in the range of 20 meters with an electric field strength of 10 V / m, the induced voltage will be about 5 V. However, the input resistance of the Hertzian dipole has a capacitive character and is large in absolute value. Resistor R3 forms a divider with this resistance, which significantly reduces the voltage across the detector. It can be calculated using the data from [3] or using the MMANA program, but it is still better to calibrate the meter experimentally on each of the used ranges. The resistance of the resistor R3 in this case can be much larger. Literature
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