This circuit was observed in an aged edition of "73 Radio Electronics". Construction was undertaken, yet performance was unsatisfactory, prompting alterations to specific components for enhanced sensitivity.
This circuit design represents a relatively uncomplicated configuration. The initial stage functions as a crystal receiving circuit. A germanium detector diode – such as the 1N34, though the AA119 diode is frequently encountered across Europe – is essential; silicon diodes are unsuitable for this purpose. The operating frequency is controlled by the values of the inductor (L) and capacitor (C). For FM band and VHF operation, a coil with a diameter of 5mm and 6-8 turns of coated wire measuring 1mm in thickness is recommended. The frequency can be fine-tuned by adjusting the spacing between the coil windings, either increasing or decreasing the gap. The capacitor’s value is less critical, with approximately 100pF being a preferable choice.
The second stage leverages the adaptability of the 2N3819 JFET, a high-impedance amplifier known for its versatility. The 470k potentiometer allows for fine adjustment of the circuit’s sensitivity. A trimmer capacitor is employed for calibration and zeroing the meter. A standard 50mA or slightly smaller ammeter, sourced from a salvaged electronic box, can be utilized for measurements.
Acceptable performance levels cannot be anticipated from this uncomplicated detector-based meter. The sensitivity is sufficient for a rudimentary assessment of the power output produced by a transmitter.
The field-strength meter is particularly useful for determining the optimal operating power of a transmitter. It proves advantageous during stage alignment, as frequently seen in configurations such as the 4W transmitter, or when exploring varied antenna designs.