AM Receiver. From DC to 1.8 MHz RADIO&TELEVISION

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RDIO&TELEVISION M Receiver From DC to.8 MHz Design by G. Baars Not all M receivers are created equal. The receiver described here is definitely not a run-of-the-mill type. The tuning range is not limited to the medium or long wave bands but extends down to extremely low frequencies. This opens up new possibilities. The receiving range of the receiver described here is continuously variable from DC to.8 MHz. That makes this receiver special, since most M-receivers are only suitable for the long wave band (50-4 khz) and the medium wave band (approximately 50-6 khz). What does this widened range have to offer? Those who live near the coast will especially appreciate the extra section from 600 to about 800 khz. Several coast guard stations operate in this range and these often provide very interesting information, usually weather conditions. t the low end of the tuning range, particularly the so-called VLFband from 9 to 48.5 khz enjoys increasing interest. The activity within this range includes, among other things, communications with submarines. Several services also operate on these super low frequencies, including teleprinter (RTTY) stations, meteorological services and the famous time transmitter DCF77 (on 77.5 khz). For the enthusiast, the VLF-band is a fascinating range. Table offers a sampling of the stations that operate in this band. Double Superhet First a brief overview of the receiver. Because of our requirements regarding sensitivity and selectivity, the receiver has been designed as a double superhet. For those who would like to refresh their memory of what a superhet, or more precisely, superheterodyne receiver, exactly is, are referred to the sidebar. For the antenna, a very short vertical was selected; a length of 0 cm suffices! Tuning of the receiver is achieved with a potentiometer and a varicap diode. The filters employ only standard ceramic filters and ready-made E-chokes. There is no need to wind any coils! lot of people will normally shy away from winding coils for themselves. They will applaud the fact that, in this respect, the receiver is very easy to build. In addition, it can be reported 46 Elektor Electronics /00

RDIO&TELEVISION that the receiver is quite integrated, consisting mainly of three ICs, supplemented with a handful of standard parts. nd finally, because the adjustment is limited to a single trimmer, anyone with at least moderate soldering skills can be expected to successfully construct the receiver on the specially designed PCB. Blocks in a row We limit ourselves first to the description of the block diagram, because this way it will quickly become clear how all the pieces of receiver work together. s shown in Figure, the received signal, with a frequency of 0 to.8 MHz, arrives at an amplifier stage, continues on to be filtered and is fed to a mixer. Here, it is mixed with the signal from a variable oscillator with a frequency which is 0.7 MHz higher than the received signal. This variable oscillator is used to tune the receiver. The difference signal resulting from the mixing operation has a fixed frequency of 0.7 MHz (the first intermediate frequency). This signal is, once again, amplified and filtered and applied to another mixer. This time with a signal from a fixed oscillator at 0.45 MHz. The mixer difference signal (the second intermediate frequency) has a frequency of 455 khz and is also filtered, amplified and finally demodulated. The signal then arrives, via a low pass filter, at an audio frequency amplifier that raises the signal to loudspeaker level. The line that starts behind the demodulator and runs back, via a low pass filter, to the intermediate frequency amplifiers is part of the GC (automatic gain control) circuit. This controller ensures that during the reception of strong broadcast stations, the amplification of the intermediate frequency amplifiers is reduced so that strong stations and weak stations will appear nearly equally loud. Schematic It is now time to look at how the various blocks are realised in practice. Figure depicts the complete Table 9.0 to 48.5 khz Some Utility Stations Freq. (khz) Call Description 8. UNID Teleprinter 5.6 RTO Moscow Meteo 60.0 MSF Rugby TS 75.0 HBG Nyon TS 77.5 DCF77 Mainflingen TS 8.8 MKL RF Edinburgh. SO Warsaw Meteo 7.4 DCF7 Offenbach Meteo 9. DCF49 BMPT Bonn 9.0 TB TN nkara 47. DDH47 Hamburg Meteo schematic diagram for the receiver. dual gate MOSFET (T) is used for the input amplifier. The most important function of this stage is impedance matching this is because we choose a very short and therefore high impedance antenna. This is followed by a low pass filter, which eliminates signals above Superheterodyne The earliest receivers consisted of little more than a tuneable RF stage for transmitter selection and a detector. When the number of broadcast transmitters increased, it quickly became clear that a single RF stage was insufficient to separate the stations. To increase the selectivity, a second RF stage was added. Such double tuned radio frequency (TRF) receivers (Figure ) were popular for a long time. But eventually, the double TRF also failed to provide sufficient selectivity. Of coarse, the concept can be extended to three, four or five stages, but all the LC tuned circuits have to be synchronously adjusted. This is not a trivial task. The arrival of the superheterodyne receiver (Figure B) resulted in a huge step forwards. The trick is to mix the input signal with a variable oscillator, which is synchronously adjusted with the RF stage (by using two variable capacitors on one spindle, just as with a double TRF). The oscillator frequency is chosen such that the difference between the input- and oscillator frequencies is constant. In the example of figure, when the input frequency changes from 500...600 khz, the oscillator frequency changes simultaneously from 955 055 khz. Therefore, independent of the selected input frequency, the difference frequency (the intermediate frequency) will, after mixing, always be 455 khz. The advantages are clear. To increase selectivity, as many stages as are desired may be added after the mixer, without the need to tune them synchronously with the input stage. They can simply be of fixed frequency (455 khz in this example). The superhet is often extended to a double superhet, by adding another mixer and oscillator. This results in a further increase in performance. 500... 600 khz 955... 055 khz MIX OSC. about MHz. This filter, consisting of L, L/C6, C7 and C8, has been designed in such a way that it provides an extra notch at the second intermediate frequency of 455 khz. Practical experience shows that some stations have significant residual field strength at this frequency. s can be observed, the filtered signal is applied to pin of IC. This IC (type 455 khz 00076-00076 - 4 B /00 Elektor Electronics 47

RDIO&TELEVISION 0....8 MHz MHz 0.7...5 MHz MIXER 0.45 MHz 0.7 MHz 455 khz MIXER Figure. Block diagram of the double superhet configured M-receiver. S6N) consists of a balanced mixer and an oscillator and is ideal for the first mixing ceremony. The ring oscillator is connected to pins 6 and 7. It is dimensioned such that the oscillator frequency, with the aid of varicap diode D and multi-turn potentiometer P, can be varied from 0.7 to.5 MHz. P, therefore, serves to tune the receiver. We would like to quickly add that the choice of varicap diode D is extremely critical. The MV40 has a capacitance variation of 0-600 pf when the tuning voltage ranges from to 0 V; a device with different capacitance will result in a change of the receiver frequency range. 0.7 MHz band pass filter follows the first mixer. This filter provides the desired 00076 - selectivity and also removes the undesirable frequencies resulting from the mixing process. We are only interested in the difference signal between the oscillator and the input frequency (.5 MHz.8 MHz = 0.7 MHz) and not the sum (.5 MHz +.8 MHz = 4. MHz). Emitter follower T provides impedance matching from the output of the 0.7 MHz filter and the input of IC. This IC, a TD57, takes care of practically all the remaining functions in the block diagram. In fact, the TD57 is a complete integrated M-receiver circuit. It contains, among other things, a mixer, two IF amplifiers with GC control and a demodulator. The 0.7 MHz signal is first amplified and then mixed with a (fixed) 0.45 MHz oscillator, resulting in a second intermediate frequency of 455 khz. This signal is amplified again, then filtered with the aid of a ceramic filter, demodulated and routed to the output via a low pass filter. The required oscillator signal is generated with the circuit around FET T4. The crystal used here has a screened enclosure, which has to be grounded. The advantage of this external oscillator is that there is no need to adjust it. part from the ceramic 455 khz filter (X) and a few compulsory passive components (mostly capacitors), the circuitry around T and D is the only external circuit. This is a simple tuning indicator, the sensitivity of which can be adjusted with P. The demodulated signal is available on pin 9 of IC. C forms part of a low pass filter, after which the signal via C and volume control P is presented to a small IC audio amplifier. The well-known LM86 is used here; it can provide a few hundred milliwatts at full output to a 9V 6V L6 8µH X SFR455H C4 R k D R8 C 0p R M C 00k 00k R T R 80Ω k R5 C5 C4 0n BF96 R4 C L 00µH C6 56p L µh9 L 00µH C7 80p C8 56p k8 C 8 C9 4 IN OUT 0n IC S6N 5 IN B OUT B OSC OSC R6 C0 7 66 0n R9 k X 0M7 0k C R C9 0n BF494 R0 k7 00Ω L5 680µH C 0p T C0 7 0n R 4 5 C 0p C5 47µ 6V IC TD57 5 4 8 6 4 5 6 7 8 L7 µh C6 C7 C8 C9 C4 C0 C Ω k5 P R6 0k 0 9 80k R7 BC550C C C T V 46m BF96 G D N400 S C8 0µ 6V G D V 9V 6V IC4 78L09 C9 0µ 6V IC5 78L06 C40 0µ 6V C8 6V k9 C4 C 00p p P 50k R7 C6 50k MT 00p R8 C5 C7 D 40p MV40(BH) C p L4 µh5 J0 D G S X 0k R9 C44 C4 9p C4 00p 9V T4 J0 R0 k C5 0p 0n 0V P 50k log 0n 0n C4 µ 6V IC 6 8 4 7 LM86N µ 6V 5 R4 Ω µ 6V C7 C6 0µ 6V n V LS LS 8 Ω W 0.45MHz 00076 - Figure. The size of the circuit is small as a consequence of a special M-receiver IC (IC) 48 Elektor Electronics /00

RDIO&TELEVISION C7 C L4 D C6 IC R9 C7 L R0 R6 R4 C9 R7 C9 C6 C9 T T C8 H R C0 R8 IC4 X T4 C4 C4 X X R9 R C5 C C7 C R D C L7 R0 L L R IC C6 00076- T C0 C8 C9C4 C0 R6 C8 C P C C4 P L5 L6 H R5 C4 C6 C T C C C5 C40 P C4 C C R R C8 IC5 C44 R7 C5 C5 C H R4 D C7-67000 LS IC H4 0 R8 ROTKELE )C( T + C4 00076- (C) ELEKTOR Figure. The cleverly designed PCB layout makes construction a simple task. /00 Elektor Electronics 49

RDIO&TELEVISION small 8 Ω loudspeaker. This is sufficiently loud for living room use. Finally, a few remarks about the power supply. There are three power supply voltages: V, 9 V and 6 V. normal V mains adapter may be used, the voltage of which is applied directly to the audio amplifier, IC. Voltage regulator IC4 provides a stable 9 V for IC, and the remainder of the receiver runs from the stabilised 6 V generated by IC5. Construction The construction of radio-frequency circuits is traditionally a little more critical than low frequency or digital designs. However, the construction of this receiver is remarkably easy and the few critical areas have been carefully considered during the PCB layout stage. In this case that means, for instance, short tracks around T and the oscillator connections of IC, decoupling via the shortest possible paths to ground, and generally a lot of copper that functions as a ground plane. There remain, therefore, very few problems for the builder. It can confidently be said that, if you do a tidy job of the soldering and stick to the parts list of Figure, very little can go wrong. Pay careful attention to the polarity of semiconductors and other polarised components. This applies in particular to T: the short leg with the protruding part (source) connects to C and the longest leg (drain) to C4. The coils are, without exception, standard chokes shaped like resistors that makes it easy. The input of filter X is marked with a black dot; this side connects to R9. X possesses an asymmetrically placed pin, which makes getting it wrong almost impossible. Crystal X has no centre leg. The third leg is made by (quickly!) soldering a short piece of bare wire to the crystal. The dimensions of the PCB are such that it fits nicely in, for instance, a Bopla enclosure type E440. Because both potentiometers are also fitted on the circuit board, wiring is a simple affair: only the antenna and loudspeaker need to be connected. The lengths of the potentiometer spindles and the leads of LED D need to be selected in such a way as to enable them to protrude through the front of the enclosure. The power supply for the receiver can be a standard V mains adapter; since the power consumption is barely 50 m there are no further requirements. djustment and Usage The adjustment is limited to the calibration of COMPONENTS LIST Resistors: R = MΩ R,R = 00kΩ R4 = kω R5 = 80Ω R6 = kω8 R7 = 50kΩ R8 = kω9 R9 = kω R0 = kω7 R = 0kΩ R = 00Ω R = Ω R4 = Ω R6 = 0kΩ R7 = 80kΩ R8,R0 = kω R9 = 0kΩ P = 50 k 0-turn cermet P = 50 k logarithmic potentiometer P = kω5 preset Capacitors: C,C,C5 = 0pF C,C,C5,C,C7,C8,C,C4,C 6,C7,C,C6,C44 = F C4,C9,C0,C8,C9 = 0nF C6,C8 = 56pF C7 = 80pF C = pf C = pf C4,C6,C4 = 00pF C5 = 40pF trimmer C9,C0,C4 = 0nF C = 0pF C5 = 47µF 6V radial C0 = µf 6V radial C,C4 = µf 6V radial C = nf the oscillator range using C5. The simplest method is as follows. Temporarily short circuit the antenna connection (point ) to ground and turn tuning potentiometer P fully to the left. Then, slowly adjust C5, starting at the centre position, until a signal is observed; the oscillator is now exactly at 0.700 MHz. You may also use a frequency counter to adjust the signal on pin 7 of IC to 0.700 MHz. The disadvantage however, is that the measuring instrument presents a small load and causes a change in frequency. This can be prevented by temporarily connecting a 0 kω resistor from pin of IC to ground; this causes a buffered version of the oscillator signal to appear on pin 5 of IC. The vertical antenna can now be C7,C8 = 0µF 6V radial C9,C40 = 0µF 6V radial C4 = 9pF Inductors: L = µh9 L,L = 00µH L4 = µh5 L5 = 680µH L6 = 8µH L7 = µh Semiconductors: D = MV40 (Motorola)* D = N400 D = LED high-efficiency T = BF96 T = BF494 T = BC550C T4 = J0* IC = S6N (Philips Semiconductors)* IC = TD57 IC = LM86N IC4 = 78L09 IC5 = 78L06 Miscellaneous: LS = miniature loudspeaker 8Ω watt X = 0M7* ceramic filter X = SFR455H* ceramic filter X = 0.45 MHz quartz crystal Enclosure: e.g., Bopla type E440 PCB, order code 00076- (see Readers Services page) *) suggested supplier: Barend Hendriksen, website at http://www.xs4all.nl/~barendh/ Email: barendh@xs4all.nl connected and the test drive can commence. The prototype was found to be very sensitive and selective. In addition to the British broadcast stations, Dutch German, French and Belgian stations were received during the day. During the evening, many Scandinavian and eastern European stations were added to that. In the range below 50 khz several data stations were heard. The ideal length of the antenna is somewhere between 0 and 0 cm. longer antenna is not recommended because of increased interference levels caused by atmospheric disturbances. (00076-) 50 Elektor Electronics /00