[Footnote 8: My thanks are due to Professor D. C. Miller and to the
Macmillan Company for permission to reproduce Figs. 79 to 83 inclusive
from that interesting book, "The Science of Musical Sounds."]
LETTER 17
GRID BATTERIES AND GRID CONDENSERS FOR DETECTORS
DEAR SON:
You remember the audion characteristics which I used in Figs. 55, 56 and
57 of Letter 14 to show you how an incoming signal will affect the
current in the plate circuit. Look again at these figures and you will
see that these characteristics all had the same general shape but that
they differed in their positions with reference to the "main streets" of
"zero volts" on the grid and "zero mil-amperes" in the plate circuit.
Changing the voltage of the B-battery in the plate circuit changed the
position of the characteristic. We might say that changing the B-battery
shifted the curve with reference to the axis of zero volts on the grid.
[Illustration: Fig 56]
[Illustration: Fig 63]
In the case of the three characteristics which we are discussing the
shift was made by changing the B-battery. Increasing B-voltage shifts
characteristic to the left. It is possible, however, to produce such a
shift by using a C-battery, that is, a battery in the grid circuit,
which makes the grid permanently negative (or positive, depending upon
how it is connected). This battery either helps or hinders the plate
battery, and because of the strategic position of the grid right near
the filament one volt applied to the grid produces as large an effect as
would several volts in the plate battery. Usually, therefore, we arrange
to shift the characteristic by using a C-battery.
[Illustration: Fig 85]
Suppose for example that we had an audion in the receiving circuit of
Fig. 63 and that its characteristic under these conditions is given by
Fig. 56. I've redrawn the figures to save your turning back. The audion
will not act as a detector because an incoming signal will not change
the average value of the current in the plate circuit. If, however, we
connect a C-battery so as to make the grid negative, we can shift this
characteristic so that the incoming signal will be detected. We have
only to make the grid sufficiently negative to reduce the plate current
to the value shown by the line _oa_ in Fig. 85. Then the signal
will be detected because, while it makes the plate current alternately
larger and smaller than this value _oa_, it will result, on the
average, in a higher value of the plate current.
[Illustration: Fig 86]
You see that what we have done is to arrange the point on the audion
characteristic about which the tube is to work by properly choosing the
value of the grid voltage _E_{C}_.
There is an important method of using an audion for a detector where we
arrange to have the grid voltage change steadily, getting more and more
negative all the time the signal is coming in. Before I tell how it is
done I want to show you what will happen.
Public-domain text, read in full here on John Shaqi.
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