05.04.2013 Views

Solid State Shortwave Receivers For Beginners - The Listeners Guide

Solid State Shortwave Receivers For Beginners - The Listeners Guide

Solid State Shortwave Receivers For Beginners - The Listeners Guide

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

It will probably not be immediately apparent why it is necessary<br />

to have a gain control for Tr2. <strong>The</strong>re are two very good reasons for it.<br />

Firstly, with Tr2 biased for maximum gain there is sufficient regeneration<br />

at some frequencies to cause the set to oscillate, even with VC2<br />

adjusted for minimum capacitance. When this occurs, VR1 can be<br />

adjusted for slightly lower gain so that A.M. transmissions can be<br />

properly resolved by the receiver.<br />

Secondly, the high gain of Tr2 makes fine setting of the reaction<br />

level rather difficult using VC2 alone. VR1 can be used as a fine<br />

regeneration control, rather in the same way as the regenerative receiver<br />

described in Chapter 2 had a fine regeneration control. Note however,<br />

that there is a slight difference in the use of the fine reaction controls<br />

on these two sets. On the regenerative receiver of Chapter 2, the fine<br />

reaction control was kept turned well back in order to give efficient<br />

detection. Here this control has no effect on the detection efficiency,<br />

and it should be kept well advanced (where possible) in order to give<br />

a high level of gain.<br />

<strong>The</strong> use of a dual gate MOSFET produces a circuit which can<br />

handle quite high signal levels without overloading. On the other hand,<br />

the set is extremely sensitive, and it is not completely immune to<br />

overloading. If an overload should occur, it will probably be possible<br />

to cure this by backing off VR1 and advancing VC2 somewhat.<br />

Detector and A.F. Stages<br />

<strong>The</strong> output from Tr2 is fed to detector diode D1 via D.C. blocking<br />

capacitor C4. C5, R5 and C6 form a very effective R.F. filter.<br />

<strong>The</strong> audio stage is a high gain common emitter amplifier using<br />

Tr3. This has R7 as its collector load resistor and R6 as its base bias<br />

resistor. C7 couples the output signal to SK3, which can be used to<br />

feed any type of medium to high impedance headphones.<br />

S1 is the on/off switch and C7 is an A.F. supply decoupling<br />

capacitor.<br />

Some readers may be wondering why it is necessary to use a<br />

separate diode detector, rather than simply use Tr2 as a regenerative<br />

detector. It would be quite possible to do this, and such an arrangement<br />

would work very well, but using a separate detector does have a<br />

couple of advantages. Furthermore, using a separate detector does not<br />

greatly increase the cost or complexity of the receiver.<br />

<strong>The</strong> bigger of the two advantages is that MOSFETs generate<br />

rather a lot of noise at A.F. If Tr2 were to be used as a regenerative<br />

detector, this noise would be coupled to the audio stages of the set.<br />

With the set up used here, the diode detector blocks virtually all the<br />

54

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!