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
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<strong>The</strong> output of Tr1 is developed across R1, and some of this<br />
output is fed to the third winding on T1. This provides the regeneration<br />
for the circuit, and VC2 is the regeneration control. <strong>The</strong> signal is inverted<br />
between the gate and drain of Tr1, and so it is necessary to connect T1<br />
with the phasing shown, so that it also inverts the signal, and provides<br />
positive rather than negative feedback. <strong>For</strong> this reason it is essential that<br />
the connections to the windings of T1 are as shown in the circuit diagram,<br />
and that, for instance, the connections to pins 5 and 2 of T1 are not<br />
reversed.<br />
<strong>The</strong>re must be a low level of loading on the output of Tr1 at radio<br />
frequencies by theaudio circuit, or it may be found that sufficient regeneration<br />
cannot be obtained. R.F. choke L1 has therefore been interposed<br />
between Tr1 drain and the R.F. filter capacitor. L1 and C3 provide very<br />
effective R.F. filtering, but allow an easy passage for audio signals. <strong>The</strong><br />
high impedance of L1 at R.F. ensures a very low level of R.F. loading on<br />
Tr1’s output.<br />
Operational amplifiers such as the 748 I.C. used here have two<br />
inputs, a non-inverting one (+) and an inverting one (-). Normally these<br />
devices are used with a centre tapped power supply when used in the<br />
configuration employed here. <strong>The</strong> non-inverting input wouldconnect<br />
to the centre tap. In this circuit a single supply is used, and the junction<br />
of R4 and R5, in effect, forms the necessary centre tap.<br />
<strong>The</strong> voltage gain of the I.C. is extremely high, being typically<br />
some 100 dB (100,000 times!), and in a practical circuit it is necessary<br />
to use a lange amount of negative feedback between the output and the<br />
inverting input in order to reduce the gain to the required level.<br />
<strong>The</strong> most simple way of doing this is to connect the input signal<br />
to the inverting input of the I.C. via a resistor which has a value which<br />
is equal to the desired input impedance of the amplifier. <strong>The</strong> inverting<br />
input forms what is termed a ‘virtual earth’, and so the input impedance<br />
of the circuit will be approximately equal to the value given to this<br />
resistor. A resistor having a value equal to that of the required voltage<br />
gain multiplied by the value of the input resistor is connected between<br />
the output and inverting input of the I.C.<br />
Unfortunately, this simple arrangement is often unsatisfactory<br />
when a fairly high voltage gain is required, as it is here. This is because<br />
the feedback resistor has to be extremely high in value, and this can<br />
seriously upset the D.C. biasing of the amplifier. To overcome this<br />
problem the feedback resistor has been made up from two resistors<br />
in series (R6 and R7), and these have a low enough combined value<br />
to provide stable D.C. biasing. Some of the A.C. feedback is decoupled<br />
by R8 and C8, and this boosts the gain at audio frequencies to the<br />
required level.<br />
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