A COMPLETE SIMPLE OSCILLOSCOPE
The oscilloscope described here is a simple one and therefore
limited in its application. It has been designed, however, to
include a two-speed time-base, derived from the 6.3 volts 50
cycles heater supply. This timebase will enable repetitive
wave-forms at frequencies between about 150 and 10,000 c/s to be
examined. Synchronisation is not possible with a simple 50 c/s
time-base but it will be found quite easy to "hold" a
display long enough for close examination or for photography,
particularly at the lower frequencies. When the internal 50 c/s
time-base is switched off, the valve used for its formation,
becomes an amplifier with the X input connected to the grid. An
external "linear" time-base can therefore be connected
to the X terminals. Otherwise any repetitive wave-form may be
connected to the X input and its amplitude controlled by the
"sensitivity'' control. Simultaneously any wave-form may be
connected to the Y input terminals for display in conjunction
with either the time-base or with any signal applied to the X
input. Provision is therefore made for Lissajous pattern work
(frequency comparison as outlined earlier).
The Y shift-control (VR4) has been incorporated to provide just
sufficient movement of the spot to keep the display centered. A
brilliance control has been included also, but this is
inoperative when the time-base is in use (VR3). In this case the
brilliance level is fixed by the application of a 50 c/s voltage
to the c.r.t. cathode which serves primarily to prevent the
flyback trace appearing. The additional socket marked r.f. is
a.c. coupled via an isolating capacitor, to one Y plate. The
socket may be used for direct injection of an r.f. carrier when
it is required to examine a modulation envelope, etc. This
facility may be used with or without the time-base.
The response of the Y amplifier is linear between 10 and 30,000
c/s, the response of the X amplifier, when not used for the
time-base, being approximately the same.
Circuit Details. The d.c. supply for both c.r.t. and valves is
derived from a bridge rectifier connected across the secondary of
the mains transformer. The secondary voltage a.c. should be
between 300 and 350 volts although a voltage below 300 could be
used with some loss of brilliance on the c.r.t.

As the circuit diagram shows, only two valves are used, one as
a Y-plate amplifier (VI = EF86 or 6BW7) and the other as a
combined time-base and Y-plate amplifier (V2 = 12AX7) or
equivalent. This is a twin triode with its front half (V2A)
switched as either time-base or X amplifier with the second half
(V2B) used as a phase-splitter to feed a symmetrical voltage to
the X plates.
The time-base is a rather novel one employing a 6.3 volts a.c.
drive to V2A grid, so that the valve is over driven. Negative
feedback helps linearise that part of a cycle used for the actual
X scan. The speed of the time-base is controlled by the series
resistors R7 and R8. For full operation as an X amplifier, the
a.c. supply to the grid of V2A is switched off and the anode to
grid negative feedback disconnected. The 50 c/s voltage for both
time-base and c.r.t. flyback suppression is derived from the
heater supply, one side of which must be earthed as shown in the
circuit. The cathode-ray tube chosen for this simple oscilloscope
is the Mullard DH-3-91 which is a 1 in. diameter tube with
internal focus control. (Connections for tube and base are shown
in Fig.)

N.B. The tube must be orientated so that pin 5 of the base is
uppermost as shown. The X plates will then be in the correct
position for horizontal scan.
Layout and Construction.
The layout of the oscilloscope is not critical since the circuits
are simple. The mains transformer must, however, be clear of the
c.r.t., otherwise 50 c/s trace modulation is liable to occur. The
tube could, of course, be fitted with a mu-metal sleeve to
obviate this, but prevention is always better than cure. In the
prototype model shown in the photograph of Plate 16 the mains
transformer was mounted about 6 in. from the tube and carefully
orientated until no modulation of the spot or a trace was
visible.
In the prototype, the valves were mounted one either side of the
tube, most of the small components being mounted on tag-panels
beneath the chassis, with larger components above.
THE DH3-91 CATHODE-RAY TUBE
These tubes are made by Mullard Limited and further details are
obtainable from Mullard Limited, Mullard House, Torrington Place,
London, W.C.2. It may not be possible to purchase them from
radio-component dealers but a dealer should be able to obtain
them without difficulty from his regular wholesaler.
The DH3-91 trace is green and has a medium persistence. The X
plates are suitable for symmetrical operation but the Y plates
are suitable only for asymmetrical operation. An internal
electrostatic system is used for spot focus. The tube may be
supported on the base but care should be taken to minimise the
effects of shock.
It is unwise to allow full brilliance when the spot alone is
displayed, as there will be a risk of burning a small dark hole
in the screen. Normal operating conditions of the tube are as
follows but note that deflection sensitivity will be slightly
lower if the operating voltage of 500 volts maximum is exceeded.
| Voltage - A1 + A3 + Y2 | + 500 volts |
| Voltage - Grid (The Grid must not be allowed to run positive.) |
- 8 to - 27 volts |
| Sensitivity X | 0. 19 - V |
| Sensitivity Y | 0.22 - V |
| Line width | 0. 6 - V |
Owing to the presence of a transparent conducting film connected
to the anode and which lies between the screen of the tube and
the glass, the tube may be operated with its cathode at earth
potential, otherwise oscillogram distortion may occur when an
earthed body is brought near the screen.
The prototype oscilloscope performed well and both sine and
square waves could be displayed without distortion. The frequency
limitation for square waves is, however, approximately 20 c/s to
15,000 c/s.
The frequency range of the X and Y amplifiers and the range of
the 50 c/s time-base are more than adequate for checking
audioamplifiers, etc. Frequency comparison by the Lissajous
method can be carried out at radio frequencies by using the r.f.
input socket for one source and a connection to the one of the X
plates, via a 0.001 uF. mica capacitor. If work of this nature is
envisaged an additional socket could be fitted and the capacitor
permanently connected to an X plate, as has been arranged for the
Y input.
Components.
The brilliance (VR3) and shift (VR4) controls may be standard
type pre-set potentiometers such as those used in television
receivers. A panel-mounting type should be used so that the small
control knob protrudes through the front panel.
The X and Y gain controls VR2 and VR1 respectively are standard
type carbon potentiometers and the time-base switch is a
three-pole, three-way type on a single wafer (S1 S2 and S3). All
other components are marked on the circuit diagram and should be
readily obtainable from most radio-component dealers.