Oscillator Board
Front Panel5
Wow & Flutter Board5
Pot. Mounting Board6
Distortion Meter Board6
Millivoltmeter Board7
Power Board7
Rear Panel8
W&F Mother Board8
Oscillator Mother Board8
Millivoltmeter Mother Board8
1. TECHNICAL SPECIFICATION
1.1 OSCILLATOR
Frequency Range
15Hz to 150kHz in four ranges
Frequency Response
Flat within ± 0.2dB over the range 15Hz to 150kHz
Distortion
Less than 0.025% at 1kHz
Less than 0.08% over the range 100Hz to 20kHz
Maximum Output Level *
3V (approx.) into open circuit
Not less than +8 dBm into 600 ohm load
Output Attenuator
Coarse- Six steps of 10dB
Fine- Continuous over range of 15dB approx.
External - Fixed 40dB
Output Impedance
Independent of frequency
Dependent on setting of output attenuator coarse control:
always less than 450 ohms. From external 40dB attenuator 47 ohms
1.2 WOW & FLUTTER OSCILLATOR
Frequency
3.15kHz(Suffix A models, 3kHz)
Output Level
350mV approx.
Output Impedance
220 ohms approx.
1.3 MILLIVOLTMETER
Frequency Response
Flat within ± 0.2dB over range 10Hz to 150kHz
Accuracy
Within ± 2% f.s.d. over range 30Hz to 20kHz
Sensitivity
1mV to 100V f.s.d. in 11 steps of 10dB
* With the addition of an Auxiliary Test Set Unit, up to +20dB into 600 ohm load.
Input Impedance
2 Megohms (approx.)NOTE :No D.C. path between the input leads.
Indication
Average reading meter scaled in romose values for sinusoidal signals
1.4 WOW & FLUTTER METER
Type of Measurement
Meter measures peak wow and flutter weighted to DIN 45507
Input Signal Required
3.15kHz (Suffix A models 3kHz) at level not less than 7SmV
Normally this is supplied by the Fixed Frequency Test Signal Generator of the Test Set itself
(see 1.2 above)
If the test signal is from another source, e.g. a pre-recorded test disc or tape, then the
frequency of the test signal should be within t 5% of the nominal value.
Sensitivity
Three ranges for wow and flutter measurements :0.1%,0.3%& 1% fsd
One range, direct reading for drift measurements : t 2% fsd.
Input Impedance
50,000 ohms approx.
Frequency Response for Wow and Flutter Measurements
Maximum at 4.0Hz : 6dB points at 0.8Hz and 20Hz
Alternative Output
The signal measured by the meter also appears on a BNC socket on the front panel and can
be fed to an external oscilloscope, wave analyser, filters, etc.
The output level is 3V (approx.) for meter f.s.d. from a source impedance of 15,000 ohms.
1.5 DISTORTION METER
Type of Measurement
Rejection of fundamental by a tuned filter.
Input Signal Required
Frequency within the range 400 to 1100Hz (approx.) Signal normally supplied by the Variable
Frequency Test Signal Generator (see 1.1 above)
The level of the signal from the equipment under test should be 100mV or more. Smaller
inputs may be used but with an increased minimum distortion reading.
Second Harmonic Rejection
Less than 0.25dB
Minimum Reading (from a distortionless source)
Less than 0.05%
Bandwidth of Harmonic Distortion Measurement
15Hz to 20kHz
There is an optional L.F. cut (turnover 400Hz) for the rejection of hum and other L.F. noise
components.
Input Impedance
100,000 ohms approx.
Alternative Output
The signal measured by the meter also appears on a BNC socket on the front panel and can
be fed to an external oscilloscope, wave analyser, filters, etc.
The output level is 1V (approx.) for meter f.s.d. from a source impedance of approximately 500
ohms.
1.6 GENERAL
Power Supply
105- 120 V, 50 or 60Hz or 200 - 250 V, 50 or 60Hz; 12 watts approx.
Dimensions
17 3/8 in. (441 mm) wide
10 in. (254 mm) deep over handles
5 5/8 in. (143 mm) high
Weight
13 lb (5.9 kg) approx.
Access
Access to the inside of the case is obtained by removing two
screws from the underside of the lip above the back panel.
2. OPERATING INSTRUCTIONS
2.1 CONNECTIONS
2.1.1 Power Supply
Check whether the voltage selector at the back of the Test Set is set to the appropriate voltage
range, 105-120V or 200-250V. If it is not, pull the selector knob outwards, rotate it to the
required position and then press it home again firmly but gently. (On later models, see Section
3.3)
No adjustment for supply frequency in the range SO-60Hz (approx.) is required.
The power lead attached to the Test Set should be connected, through an appropriate plug, to
the power supply (AC only).
The Test Set is switched on and off by turning the "SUPPLY" knob at the right of the front
panel. The meter is illuminated to show when power is applied.
2.1.2 Signal
The BNC socket marked "oscillator" should be connected to the input of the equipment under
test
If the external 40dB Attenuator is required, the 'flying'
lead should be connected to the "oscillator" socket and the connecting cable to the Attenuator.
The BNC socket marked "meter" should be connected to the output of the equipment under
test.
Note 1. Cables for connecting the Test Set to the Line Input and Line Output sockets of a
Note 2. Since the Test Set has a common earth path between input and output sockets,
2.2 CALIBRATION
2.2.1 General
For this purpose it does not matter whether the Test Set is connected to the equipment
to be tested or not. It is recommended, however, that the power supply should have been
switched on for at least 5 minutes before calibration in the Drift and the Wow and Flutter
modes is checked.
Ferrograph Series 7 recorder are supplied. These leads are irreversible and
ensure that the 'earthy' sides of the Test Set and the recorder input and output
circuits are connected together. When other leads or other end connectors are
used, care must be taken to ensure that this condition still obtains.
great care should be taken to ensure that this does not result in a small part of
the audio output current flowing through the input earth. When high-sensitivity
inputs are being used, this could give rise to spurious noise or distortion
readings. These can usually be prevented by the insertion of a small resistor
(e.g. 100 ohm) in series with the "meter" input earth lead.
The adjustments are not interdependent and can be carried out individually.
2.2.2 Millivoltmeter
(1) Set the "MILLIVOLTMETER" switch to the "1V" position.
(2) Press down the "read input" button. (This releases the button to its left and the three
buttons to its right).
(3) Press down the "CALIBRATE" button.
(4) The meter pointer should now lie on the CAL mark above the outer scale; if not,
adjust the screwdriver-operated control "mV meter cal (1V range)".
(5) Press the "CALIBRATE" button to release it.
Note When this adjustment has been carried out with the "MILLI-VOLTMETER" switch in the
"1V" .position, the meter measures voltage on the top scale with full scale deflection of
1V. Movement of the "MILLIVOLTMETER" switch adjusts the meter
sensitivity to give full scale deflection for inputs of lmV to 100V, as indicated on the
switch, reading on the appropriate one of the two upper scales.
For setting the meter to read arbitrarily, see 2.3.4 below.
2.2.3 Drift
(1) Press down the "W&F drift" button. This releases the two buttons on either side
and applies a 3.15kHz * test signal to the "oscillator" socket and to the meter circuits.
(2) Press down the "CALIBRATE" and "W&F drift" buttons (thus releasing the
"1%","0.3%", and "0.1%" buttons).
(3) The meter pointer should now read 0 on the "drift %" scale; if not, adjust the
screwdriver-operated, pre-set control marked "drift set zero".
(4) Press down the "CALIBRATE" button to release it. The meter now measures drift
directly on the "drift %" scale.
2.2.4 Wow and Flutter
(1) With the "W & F drift" button still pressed (see above), press the "CALIBRATE" and
"0.3%" buttons (releasing the "drift, "1%" and "0.1%" buttons).
(2) The meter pointer should now lie on the CAL mark above the top scale; if not, adjust
the screwdriver-operated pre-set control marked "peak wow cal (0.3% range").
(3) Press down the "CALIBRATE" button to release it.
The meter now reads percentage wow and flutter (0.3% f.s.d.) on the next to top scale.
Pressing down the "1%" or "0.1%" button releases the "0.3%" button and the meter then
reads percentage wow and flutter on the top scale with f.s.d. 1% or 0.1%
2.3 MEASUREMENTS
2.3.1 Preparation
In the following it is assumed that the gain controls on the equipment under test have been set
for normal operating conditions. It is also assumed that the input and output signal voltages
under these conditions are known, at least approximately. If not, then initially the
OSCILLATOR OUTPUT coarse" switch should be set to its lowest (10mV) position and the
"MILLIVOLTMETER" switch to its highest (100V) position. When connecting to a microphone
input socket, the external 40dB Attenuator should be inserted between the Test Set and the
equipment under test (see 2.1.2)
The "OSCILLATOR OUTPUT coarse" control should then be turned clockwise, step by step,
until a proper operating level has been obtained. If this requires the "OSCILLATOR OUTPUT
coarse" control to be set higher than 3V, then the 40dB Attenuator should be removed from the
output.
With a proper output level from the equipment under test, the "MILLIVOLTMETER" switch on
the Test Set should be turned anti-clockwise step by step, until a convenient reading on the
meter is obtained.
2.3.2 Frequency Response
(1) Set the "OSCILLATOR OUTPUT coarse" switch to an appropriate position (see 2.3.1
above) and the "OSCILLATOR OUTPUT fine" control to about mid-position.
(2) Set the "FREQ" control to 100 and press down the "FREQUENCY" range button "x 10".
The Test Set is now delivering a 1kHz test signal to the equipment under test. The level of this signal
can be controlled in steps by the "OSCILLATOR OUTPUT coarse" control and continuously by the
"OSCILLATOR OUTPUT fine" control. Once set at 1kHz, these must not be varied throughout the
rest of this test.
(3) Press down the "input" button and check that the "LF cut" and "CALIBRATE" buttons are
both released.
The Test Set now measures the output voltage from the equipment under test (see Note to 2.2.2) .
(4) The frequency of the test signal is changed by means of the "FREQ" control and the range
selecting buttons below it. The output level at various frequencies is read on the meter, its
sensitivity being increased or decreased by use of the "MILLIVOLTMETER" switch (see Note
to 2.2.2)as necessary.
A plot of output voltage against frequency shows the frequency response of the equipment under
test.
Note 1.When making frequency response and similar measurements, it is usually convenient to
have the meter reading 0 on the dB scale (or some other round number) at a chosen
frequency, say 1 kHz. Normally this is done by using the "OSCILLATOR OUTPUT fine"
control to adjust the level of the input signal to the equipment under test or by fine
adjustments of its gain control.
When neither of these things can be done, as, for example, when reproducing a prerecorded tape on equipment with no output level control, the meter may be adjusted to a
convenient reference value by pressing down the "DISTORTION set 100%" button (thus
releasing the "input" button) and adjusting the meter to the required reading by use of
the "DISTORTION METER set 100%" control. The meter now indicates relative levels
e.g. in decibels, at the various frequencies but it does not, of course, read in
volts/millivolts.
The "MILLIVOLTMETER" control should only be used on the distortion meter ranges of
"0.3%" to "100%". In view of the extreme sensitivity (10011V) of the "0.1%" range, this
should not be used for reading voltages with the. "DISTORTION 100%" button pressed.
Note 2. When making frequency response measurements on magnetic tape recorders, it is
essential that the input signal level be at least 20dB below that which gives full level
recording at 1kHz. Similar restrictions on the permissible level of test signals apply to
some other types of equipment.
Note 3. When testing a tape recorder that cannot record and reproduce simultaneously, it is
necessary first to record a series of test frequencies (with a fixed input signal level) and
then to measure output levels at the various frequencies when this recording is
reproduced.
The above procedures measure the overall response of a tape recorder. To determine
whether the reproducing frequency response is correct, it is necessary to measure the
output levels at various frequencies when reproducing a standard test tape on which the
various frequencies have been recorded to the appropriate Standard.
2.3.3 Drift
(1.) Press down the "W & F drift" button and also the "drift" button under "WOW & FLUTTER".
The Test Set now delivers a 3.1.5kHz* signal to the recorder under test.
(2) Set the recorder controls so that this signal is recorded at a normal level for, say, 40
seconds. Stop the machine, and rewind the tape to the beginning of the recording.
(3) Reproduce this recording.
Note. The level of the signal reaching the Test Set should not be less than 75mV. To check this, see
Note 1 to 2.3.4.
(4) The meter now indicates directly on the "drift %" scale the percentage difference between
the frequency of the reproduced signal and the 3.1SkHz* test signal that was recorded.
* On models Suffix A the internal oscillator is set to 3kHz.
Note When testing a disc reproducer it is necessary (and when testing a tape reproducer it
may be convenient) to reproduce a test recording made on another machine. The
indicated percentage drift may then be due partly to a difference in the recording and
reproducing speeds and partly to the original signals not having been 3.1SkHz*.
2.3.4 Wow and Flutter
(1) If not already made, first prepare a test recording as in (1) and (2) of 2.3.3 above.
(2) Press down the "1%" button under the "WOW & FLUTTER" heading (releasing the "drift"
button) and reproduce the test recording (see Note 1 below).
The meter now indicates wow and flutter on the top scale; f.s.d. 1%. If the meter reading is
inconveniently small, press down the "0.3%" or "0.1%" button (releasing the "1%" button); the meter
now indicates wow and flutter on the next to top scale with f.s.d. 0.1%.
Note 1.For proper operation of the limiter (which ensures that amplitude variations do not affect
the readings), the reproduced voltage reaching the Test Set should be more than 75mV.
This can readily be checked by pressing down the "MILLIVOLTMETER read input"
button (releasing the "W & F drift" button) and determining the level from the combined
readings of the meter and the "MILLIVOLTMETER" switch (see Note to 2.2.2)After
such a level check, the "W &F drift" button must, of course, be pressed down again to
measure wow and flutter.
Note 2. For a proper measurement of wow and flutter, the frequency of the signal fed to the Test
Set should be within about ±5% of the nominal value, 3.15kHz*. When reproducing a
test recording just made on the same machine as above, it will almost always be within
the ±2% indicated directly on the "drift% scale. This may not be the case when
reproducing a test recording made on a different machine or at another time but
satisfactory measurements of wow and flutter can still be made if, when measuring drift,
the meter can be made to read within its ±2% range by use of the "drift set zero"
control.
Note 3. Readings of wow and flutter taken while the test recording is being made usually give a
fair indication of magnitude but do not give true values since speed fluctuations that
repeat in a period corresponding to the time taken by the tape to move from the record
to the replay head do not appear.
2.3.5 Distortion
For this measurement, the output signal from the equipment under test should
preferably be greater than 100mV (see Note 3 below).
The procedure is as follows:(1) Set the "MILLIVOLTMETER" switch to "1V".
(2) Set the "FREQ" control to 100 and press down the range selecting button marked "X10".
A 1kHz test signal is now delivered to the equipment under test.
(3) Press the "DISTORTION set 100%" button.
(4) Now use the "DISTORTION METER set 100%" control knob to adjust the meter to read 10
on the top scale.
(5) Press the DISTORTION read" button (releasing the "DISTORTION set 100%" button. Also
press down the "LF cut" button.
(6) Set the "DISTORTION METER BALANCE fine" control to about mid-position (vertical) and
then use the "freq-coarse" and "phase" controls to reduce the meter reading to a minimum.
During this process, the meter sensitivity should be progressively increased by means of the
"MILLIVOLTMETER" switch to maintain a convenient reading. Complete the adjustment for
minimum reading by use of the "freq-fine" and "phase" controls.
(7) The percentage distortion can now be read on the appropriate one of the two upper scales
in combination with the % markings on the "MILLIVOLTMETER" switch.
Note 1. The test signal need not be 1kHz but it should be within the range 400-1100Hz,
approximately. Otherwise, a minimum will not be obtained within the range of the "BALANCE"
controls.
Note 2. The meter reading includes signals of all frequencies between 30Hz and 20kHz except for
the test frequency and a narrow band on either side of it. It therefore includes hum and other
low frequencies. Pressing down the "LF cut" button cuts the lower frequencies progressively
below 400Hz.
Note 3. If a level of 100mV or more cannot be obtained from the equipment under test, it will not be
possible to adjust the meter to full scale deflection as in (4) above. The measurement may still
be carried out but with the "MILLIVOLTMETER" switch set below 1V, with a corresponding
allowance in the calculation of percentage and with a restriction in the lowest level of distortion
that can be measured.
Note 4. When testing a tape recorder that cannot record and reproduce simultaneously it is, of
course, necessary first to record the test signal and then to measure distortion while it is being
reproduced.
2.3.6 Signal-to-Noise Ratio
(1) With the equipment under test working at normal operating levels, measure the total
harmonic distortion on a 1kHz test signal as in 2.3.5 above.
(2) If the total harmonic distortion is less than 2%, then increase the level of the test signal by
means of the "OSCILLATOR OUTPUT" "coarse" and "fine" controls, (or, if testing a tape
recorder, the recording gain control) until the distortion is 2%.
Note : A good idea of the rate of increase of distortion with signal level can be obtained by
successively decreasing meter sensitivity and increasing signal level in steps of 10dB but, for
the final determination of distortion, the full procedure of 2.3.5 should be carried out.
(3) With the equipment under test adjusted so that total harmonic distortion of a 1kHz output
signal is 2%, press the "MILLIVOLTMETER input" button (releasing-the "DISTORTION read"
button).
(4) Adjust the "MILLIVOLTMETER" switch to give a convenient meter deflection. The reading
of the meter, in combination with the switch (see Note to 2.2.2),indicates the output level at
which there is 2% distortion.
(5) Remove the signal from the input of the equipment under test and apply a short circuit.(But
see Note 2 below).
(6) Press the "LF cut" button to release it.(But see Note S below).
(7) Increase the meter sensitivity, by means of the "MILLIVOLT-METER" switch, until a
convenient reading is obtained. The number of millivolts indicated by the combined meter and
switch readings (see Note 2.2.2) is the total noise level. The ratio of this to the voltage
determined in (3) above, is the Signal-to-Noise Ratio, usually stated in decibels.
Note 1. When determining the 2% distortion level of a tape recorder, care must be taken that the gain
controls are so set that the distortion does not arise primarily because of overloading of the
electronics. This could happen, for example, because of an excessive input level compensated
by a low setting of the recorder gain control or because of an excessive output level.
It is the condition when the distortion arises primarily in the record/replay processes that is
usually referred to when the signal-to-noise ratio of a tape recorder is quoted.
Note 2. In the case of a tape recorder, there are several different signal-to-noise ratios that may be
considered significant, according to circumstances, but in all cases it is necessary first to
determine the output level at which the total harmonic distortion of a 1kHz test signal is 2%
(see (1),(2) and (3) above).
It is with this output level that the various noise levels are usually compared. (But see Note 3 below).
The signal-to-noise levels most usually quoted are those obtained by:-
(a) recording and reproducing simultaneously with the input short circuited and using a
bulk-erased or virgin tape;
(b) as (a) but using a tape previously recorded to saturation level;
(c) reproducing only, using a bulk-erased or virgin tape;
(d) reproducing with the tape stationary.
In each case the noise level must be measured under the stated conditions.
Note 3. Signal-to-noise ratios are sometimes reckoned from the 3% rather than from the 2% total
harmonic distortion level or from a specified tape flux level.
Note 4. Signal-to-noise ratio measurements are made with various types of meter (e.g. r.m.s. or peak
indicating) sometimes with and sometimes without a frequency weighting. This Test Set
measures unweighted noise using an average reading meter scaled in r.m.s. values for
sinusoidal signals.
Note 5. When it is tape hiss or other high frequencies that are of most interest it will usually be
convenient to make the noise measurement with the "LF cut" button pressed down.
2.3.7 Gain
(1) First proceed with steps (1) , (2) and (3) of the procedure for measuring frequency
response, 2.3.2. above.
(2) Press the "MILLIVOLTMETER read input" button and then adjust the "MILLIVOLTMETER"
switch to obtain a convenient reading on the meter.
This reading, in combination with the switch, indicates the output voltage of the equipment
under test. (see Note to 2.2.2)
(3) Now, press the "MILLIVOLTMETER read osc" button. This releases the "read input" button
and connects the meter to indicate the output voltage-from the Test Set oscillator, i.e. the input
voltage to the equipment under test.
(4) Adjust the "MILLIVOLTMETER" switch to obtain a convenient reading on the meter.
This reading, in combination with the switch, indicates the input level to the equipment under
test.
The ratio of the output level (2) above, to the input level (4) above, is the gain of the
equipment. It may be expressed as a numerical ratio or in decibels.
Note : Gain can be measured at any frequency desired by an appropriate setting of the
"FREQ" control and the range selecting buttons. Care must be taken, however, to avoid
overloading. (see Note 2 to 2.3.2.above).
3. MAINTENANCE
3.1 GENERAL
No regular maintenance is necessary on the Test Set other than occasional cleaning of the
fascia and plate. A damp cloth should be used, and persistent stains may be removed using a
weak solution of a mild detergent.
3.2 REMOVAL OF BOARDS
Access to the plug-in boards is obtained by removing the two screws ('A' in Fig.12 Exploded
View) and sliding back the top panel; access to the underside is by removing the two screws
('B' in Fig.12 Exploded View) and sliding back the bottom panel. The board fixing strap is
removed by undoing one screw at each end.
With certain boards it is necessary to remove the extension spindles by undoing the grub
screws in the couplers using a 6BA Allen key. Most interconnections are by plug-in connectors
but some are by soldered connections and these will
have to be unsoldered if the board or component is to be removed completely.
3.3 POWER SUPPLY VOLTAGE SELECTION (Serial No. 4515 onwards)
On models Serial No. 4515 onwards, the rear panel voltage selector mentioned in Section
2.1.1 is not fitted and adjustment to correspond to the power supply voltage is done internally.
Access is obtained by removing the two screws ('A' in Fig.12 exploded view, Appendix 4) and
sliding back the top panel. On the power supply transformer Tl (see Fig. 10), the Brown/
White lead should be unsoldered and resoldered appropriately; tag 2 - 110V, tag 3.- 220V or
tag 4 - 240V. The Blue/White lead should remain on tag 1. The rear panel must be marked
with the new voltage.
No adjustment is necessary for supply frequency in the range 50-60Hz approximately.
4. TECHNICAL DESCRIPTION / FAULTS
4.1. OSCILLATOR (VT1-3)
The oscillator uses three transistors in a Wien Bridge circuit, comprising two gain
stages VT1 and VT2 with an emitter follower stage VT3 to provide a low impedance
output. Negative feedback for A.C. stabilisation is provided by the potential divider
network Thermistor TH1/Resistor R7 to VT1 emitter and the D.C. conditions are
stabilised with feedback via R3/R6. The frequency of the oscillator is set by the two
parts of RV20 a& b in conjunction with C8-11 and C4-7 respectively as selected
by the Frequency Range switch SW15.
TH1
HT
+ve
R1
C8 11
R4
Fig. 1. Circuit Detail - Oscillator
FAULT
High output with excessive
distortion(squared off)
No output
R7
+
a b
RV20
VT1, 2, 3
RV19
C4 7
RV10
POSSIBLE CAUSES
Thermistor TH1 faulty-open circuit (very low
ambient temperature can cause TH1 to give
this symptom).
Transistor failure
Transistor failure
Frequency calibration wrong (all
ranges)
Frequency calibration wrong (on only
one range)
Low frequency modulation on
highest freq. range (x 1000)
x 1C7 or C8
x10C6 or C9
x100 CS or C10
x1000 C4 or C11
Transistor noisy. Resistor R5 noisy.
Resistor burnt out in attenuator chain-probably
R15 or R16 N.B. This is probably caused by
DC signal fed into the oscillator output socket
from the external connection-check before
reconnecting.
4.2. MILLIVOLTMETER (VT51-57)
R143
R142 &
R141
SW6a
(60dB
attenuator)
10
VT51, 52
R158
R153
SW6b
VT56, 57
+
100
+
R175
VT54, 55
SK30
Scope
Fig. 2. Circuit Detail - Millivoltmeter
The signal is fed via blocking 'capacitor C89 and overload protection resistor R144 with R143
& R142/141 providing 60dB attenuation as selected by SW6a, which thus doubles the ranges
selected by SW6b. Zener diode MR31 protects VT51 (not normally conducting) which is a field
effect transistor giving a high input impedance. The overall gain of the first stage VT51 & 52
is determined by the feedback resistor R150, which is effectively from VTS2 collector to
VT51 emitter (source), and the exact gain (approx. 10) is set by RV152 ('mV meter cal'). The
main attenuator (R153-158) has six steps (10dB per step) selected by SW6b, and these are
doubled by the 60dB attenuator SW6a to give 11 x 10dB steps and an earthed position.
Emitter follower VT53 is a unity gain buffer stage, feeding two separate amplifier stages. The
'scope' amplifier VT56 & 57 has feedback applied by R175, and the output signal is fed to the
'scope' output except when the 'W&F drift' button is pressed. The second amplifier is the main
amplifier VT54 & 55 for the meter itself, the meter being connected as part of the negative
feedback loop in a half bridge configuration as shown. R165 provides biasing for the diodes
MR32 & 33 to help the low signal linearity, and MR34 is a protection diode. C96 improves the
extreme high frequency response.
Fig. 3.
Circuit Detail-Meter
R162
VT54
R163
R164
VT55
R167
MR33
R100
C100
C98
R165
MR34
M1
R166
MR3
R169
C97
C96
The overall frequency response of the millivoltmeter circuit on the 300mV range or lower,
should be level, but on the 1V range and higher, trimmer C83 is adjusted to give a level
response (set on the 1V range). This may be done using the RTS oscillator as a source by
pressing the 'Read Osc' button. Any leads should be removed from the 'meter' and ‘osc’
sockets to avoid the effect of their capacitance.
The steep LF cut, which is 3dB down at approx. 400Hz, is applied to the circuit in three places,
the final response being as shown in Fig. 4.
(a) Normally the coupling capacitor from VT52 collector is C87 with C88 shorted. With the
'LF cut' button pressed, C87 is in series with C88 reducing the effective capacitance and
attenuating the bass frequencies.
(b) Similarly C94 is normally short-circuit but with the 'LF cut' button pressed it is in series
with coupling capacitor C93 thus reducing the capacity and hence the bass response.
(c) Normally the emitter of VT55 is decoupled by C99 in parallel with C9S. With the,'LF cut'
button pressed C99 is removed from earth and only C95 is in circuit. This reduces the
capacity and hence the bass response.
The Wow & Flutter section has two distinct operations. 'Drift' gives an indication of the mean
freqency of the replay signal, disregarding short term cyclic variations. This facility is normally
used for checking the speed of an equipment against a known standard, the built-in W &F
oscillator being nominally 3150Hz (3000Hz- suffix A) within 1%. The short term drift could vary
by about 0.5% during use, after calibration in the morning following an initial warm-up period of
approx. 10 minutes.
'W & F' gives the facility of measuring peak frequency excursions of the signal around 3150Hz
or 3000Hz. All test sets will cover the range 3000-3150Hz for measuring wow and flutter
without modification, the difference between RTS and RTSA being merely a change in
frequency of the built-in W & F oscillator.
4.3.1. W & F Oscillator (VT11,12)
The transistors VT11/12 form a multivibrator whose frequency is set accurately by RV33;
'coarse' adjustment (such as converting from RTS to RTSA) can be made, if necessary, by
simultaneously changing the values of R34/35. Provision has been made to modulate the
frequency with a voltage inserted across R32 from the 'Cal' oscillator in order to set the peak
W & F calibration. The output is modified to a sinewave by filter C24/L1/C25 and fed to the
'oscillator' output when the 'W & F drift' button is pressed.
4.3.2. W & F Meter (VT13-20)
For accurate measurement a signal of at least 50mV should be fed to R39, when the high
frequencies are removed by C27 and low frequencies by C26. The residual carrier signal (at
about 3kHz) is amplified by VT13 so that it is able to drive the monostable multivibrator
VT14/15, resulting in a differentiated square wave at the collector of VT1S which is at the
frequency of the original signal. This is differentiated by C31 and rectified by MR1 (positive
half-cycle) and the emitter/base junction of VT16 (negative half-cycle). The pulse produced
bottoms VT16 once every cycle and the average current through VT16 therefore depends
linearly on the signal frequency only. The voltage developed across R46 is thus proportional to
this frequency. Transistor VT17 forms a buffer, emitter-follower stage followed by a parallel -T
filter to remove the carrier frequency, thus leaving the wow and flutter products and at the
same time the response is altered so that after the W & F components have passed C40/R60
the response has been tailored to the DIN weighting curve shown in Fig. 5 . The signals are
amplified by VT19 & 20 and fed to voltage doubler MR8 & 9, with the meter calibration
adjusted by RV69. The DC level at the collector of VT16 corresponds to the mean frequency,
and this is used for the 'drift' measurement, being compared via R52 to a fixed reference level
set by RV56 when the 'drift' button is pressed.
FAULTS
There are no specific faults to suggest; malfunctions can be traced by following the signals
through the circuit and comparing the waveforms shown on the oscilloscope with those shown
in the full circuit diagram.
Meter connection with
‘drift’ button pressed
R52
C37
R51
R53
C38
R49
VT17
C34
C36
R50
C35
Fig.6 Circuit Detail - Wow & Flutter Meter
M1
C40
To fixed reference
voltage (VT18)
To amplifier for
peak W&F measurement
4.4. DISTORTION METER (VT33-37)
In
set
100%
1
RV 111
2
Freq
1
+
10
Out
Fig. 7 Circuit Detail - Distortion Meter
The signal passes through potentiometer RV111 which sets the level into the dynamic emitter
follower stage VT33. This stage has unity gain with VT34Lacting as a constant current load for
VT33, the actual current being set by R113/R115. Bootstrapping through C64 is used to
improve the input impedance, and MR22 provides protection for VT33 in the event of overload.
VT33 is critical for noise and only low noise transistors should be used.
The base of transistor VT35 is a virtual earth point due to negative feedback via R124, which
sets the gain of the amplifier stage to approx. 10. VT35 acts as a phase-splitter with emitter
and collector loads, the ratio of their gains is approximately 2 :1 and set precisely by
potentiometers in the collector load 'phase' potentiometers. The outputs are fed to a Wien
Bridge having zero output at the selected frequency as
adjusted by the Balance phase and Frequency coarse/fine controls.
Pressing the '100%' button shorts out C64, thus removing the 'notch' in the response but
leaving the gain unaffected. With the 'read' button pressed the notch in the response is
reintroduced and C68 is shorted to earth, restricting the response to 20kHz. VT36 is an
amplification stage with an overall gain of approx. 10, VT37 giving an emitter follower output
via C69.
R120
R81
Fig. 8
Circuit Detail - Distortion
Meter (Wien Bridge)
RV121
R122
VT35
RV82 phase
C51
C66
R83
R86
R85
R88
coarse
RV84a
RV87a
RV84b
RV87b
fine
FAULT
NoiseVT33 is critical for noise, and only the specified transistor should be used.
Certain components are more critical for noise - R114, R116, R117, R119,
R120, R122.
Insufficient range onSet RV121 so that meter 'nulls' when RV82 is five turns from
‘phase' controlone end viz. central.
VT36
4.5. CALIBRATION (VT31,32)
The 'Call oscillator is mounted on the Distortion Meter Board and consists of a multivibrator
operating at approx. 70Hz. A 'square wave' output is taken from each collector, that from VT31
collector being used to modulate the W & F oscillator with calibration set by RV101. The output
from VT32 is stabilised further by zener diode MR21 and further reduced to give an indication
of 0dBm on 1V range of the millivoltmeter set by RV110 as a calibration standard.
The cal oscillator is only operational when the 'cal' button is pressed.
In the setting up of the RTS, it is necessary to use test instruments of sufficient accuracy to
calibrate each section to the required performance. In general these should be of the order of
ten times more accurate than the RTS, particularly the Millivoltmeter. In an emergency, less
accurate test equipment may have to be used, but the accuracy of the RTS will then not
necessarily conform exactly to specification and this must be borne in mind when making
measurements.
5.1.Test Equipment Required
(a) MillivoltmeterMV
(b) Digital Frequency MeterDFM
(c) Distortion MeterDM
(d) Oscilltor (sine wave)0
(e) OscilloscopeS
(f) Function Generator & LF Oscillator
(see Wow & Flutter 5.6.3)
5.2. Power Supply
(a) Using the Millivoltmeter MV, check that the voltage on the pin (red lead) of the Power
Supply Board is 30V dc relative to chassis; if necessary reset RV192 on the Power
Supply Board (Fig.10 )
5.3. Oscillator
(a) Set the Oscillator output controls, Coarse & Fine, to maximum (fully clockwise) and set
the dial and push button controls to give an output of 14kHz at the Oscillator output
checked by the Frequency Meter DFM.
(b) Check that the dial indicates 14kHz; if necessary reset this by slackening the grub
screw and rotating the dial to 14kHz before retightening (on later models remove the
knob cover/insert, slacken the collet nut then retighten with the dial at 14kHz).
(c) Check that with the dial set to 4kHz the Frequency Meter DFM reading is within t 5%
(3.8 to 4.2kHz).
(d) Check the frequency accuracy similarly on the other ranges.
Dial
4 kHz
40 Hz
400 Hz
40 kHz
Frequency Limits
3.8 kHz to 4.2 kHz
38 Hz to42 Hz
380 Hz to 420 Hz
38 kHz to 42 kHz
(e)Using the Millivoltmeter MV, check that the output from the oscillator with the coarse &
fine controls at maximum is greater than 2.8V (at 1kHz approx.)
(f)Check that the 'Output' control 'Coarse' operates in steps of 10dB t 0.5dB.
(g)At 0dB on the 1V range of the Millivoltmeter MV, check that the frequency response is
level at 1kHz, 15 Hz , 40Hz, 15kHz, 150kHz, within ±0.2dB
(h) Set the oscillator output to 1V at 1kHz and using the Distortion Meter DM check that the
distortion is less than .025%.
5.4. Millivoltmeter
(a) With nothing connected to the 'meter' socket and the milli-voltmeter set to the 30V
range, check that the meter reads zero; if necessary reset the meter to zero using the
adjustment at its rear.
(b) Feed the Oscillator 0 into both the RTS and the Millivolt-meter MV, setting each to the
1V range.
(c) Set the Oscillator 0 to lkHz and adjust its output to give a reading of 0.8V on the
Millivoltmeter MV.
(d) Check that the RTS millivoltmeter also reads 0.8V; if necessary adjust the preset control
'mV meter cal' RV152 on the front panel.
(e) Check that the frequency response agrees with the Milli-voltmeter MV over the ranges
1kHz to 20kHz within ± 1% and over 15Hz to 150kHz within ± 2%; if necessary adjust
trimmer capacitor C83 to give as level a high frequency response as possible.
(f) Recheck the reading of 0.8V (at 1kHz) on both meters; if necessary reset RV152.
(g) Press 'calibrate' and check that the RTS millivoltmeter reads 0dB (still on 1V range); if
necessary reset RV110 on the Distortion Meter Board (then press 'calibrate' to release).
(h) With the Oscillator 0 set to 400Hz, press 'LF cut' and check that the response is reduced
by 3dB (± 1dB).
(i) Reset the Oscillator 0 to 1kHz and adjust the output to give a meter reading of 0dB (on
1V); switching the input signal level in 10dB steps, check that on all ranges the RTS
millivoltmeter agrees with the Millivoltmeter MV within ± 2% (one division of the top
scale).
5.5. Distortion Meter
(a) It is not essential but nevertheless highly desirable that the Oscilloscope S be
connected to the 'scope' socket throughout this section, thus enabling the output to be
observed to ensure that it is signal rather than noise.
(b) Set the 'balance' controls to their centre positions ('Phase' control 5 complete turns from
one end).
(c) With the Oscillator 0 still set to 1kHz, press 'set 100V and adjust the 'Sensitivity' control
to give full scale reading on the 1V range.
(d) Press 'read' &'LF cut' and adjust the pre-set phase control RV121 on the Distortion
Meter Board together with the 'freq coarse' & 'fine' controls on the front panel alternately
to give minimum reading, reducing the milli-voltmeter range as required.
(e) If necessary, the final reading can be obtained using the 'phase' control on the front
panel, but this must not be more than two full turns from its centre position.
(f) The final reading should be less than 0.025% (assuming that the inherent distortion of
the Oscillator 0 is much less than this).
Note: Modification of RTS2 Distortion Measurement Frequency
The frequency range of the RTS2 distortion measurement can be modified to operate at a
different frequency instead of the normal 400-1100Hz approximately by altering the value of
C51 & C66 simultaneously. In practice the value of these capacitors is not critical, but they
must have the same value within 1%. A suggested table of values is given below; values to
give other frequency ranges can be determined by proportion.
C51& C66
0.33mF
0.22mF
0.1mF
.056mF
.033mF
.022mF
.01mF
5600 pF
3300 pF
*Because of the low frequency of operation after this modification has been carried out, the 'LF
cut' button must not be pressed while making distortion measurements. The residual reading
obtainable will therefore depend upon the level of hum, etc., in the signal and this will
determine the minimum percentage distortion which can be read, although this will normally be
adequate for most 'off tape' measurements.
(a) Connect the Digital Frequency Meter DFM to the 'oscillator' output, press 'W & F drift'
and check the frequency of the W & F oscillator; if necessary adjust RV33 on the W & F
Board to set the frequency to 3150Hz (or 3000Hz) ± 1%.
Note: If RV33 does not give enough adjustment, alter the values of R34/R35 simultaneously
to bring the frequency within range (about 5-10% each should be sufficient), increasing
the value to reduce the frequency and vice versa.
(b) Connect the Millivoltmeter MV to the 'oscillator' output and check that the output is
350mV or greater ; if necessary tune Ll on the W & F Board for maximum output.
5.6.2. Drift
(a) Connect the Oscillator 0 and Digital Frequency Meter DFM in parallel across the 'meter'
input and set the Oscillator 0 accurately to 3150Hz (or 3000Hz).
(b) Press 'W & F drift' and 'drift', and adjust the 'drift set zero' control RV56 to give zero drift
on the meter (centre scale).
(c) Set the Oscillator 0 to ± 1% (3181.5Hz or 3030Hz) then to -1% (3118.5Hz or 2970Hz),
and check that the meter reads accordingly; if necessary adjust the drift sensitivity
potentiometer RV54 on the W& F Board to indicate ± 1% on the RTS meter scale.
(d) If RV44 has been adjusted, recalibrate zero drift as in (b) above and repeat (c); the
settings of RV54 & RV56 are interdependent and (b) & (c) must be repeated alternately
until no further adjustment is necessary.
(e) Remove the connections to the 'meter' socket on the RTS and press 'calibrate' (in
addition to 'W & F drift').
(f) Check that the meter reads zero (centre scale); if necessary adjust 'drift set zero' pre-
set control.
5.6.3. Wow & Flutter
(a) Connect to the RTS 'meter'• input a sine wave of 3150Hz (or 3000Hz) frequency
modulated to 0.3% peak by a 4Hz sine wave; this can be obtained from a function
generator and low frequency oscillator or another function generator.
(b) Press '0.3%' and check that the meter reads 0.3%; if necessary adjust the pre-set
control 'peak wow-cal (0.3% range)' RV69.
(c) If available, connect the Oscilloscope S to the 'scope' socket and check that a
sinusoidal wave form is shown.
(d) Press 'calibrate' and check that the meter reads on the 'cal' mark; if necessary, adjust
the cal control RV101 (lower left) on the Distortion Meter Board.
Where it is found necessary to change an electronic component, the RTS2
should be checked and re-calibrated using test equipment which is several
times more accurate than the Test Set itself. If this equipment is not
available or if difficulty is experienced, the relevant P.C. board(s) can be
sent for checking or replacement to the Ferrograph !Replacement Board
Service!.
When returning the board(s) to the appropriate overseas agent, or in the
U.K. to theU. K. SERVICE DEPARTMENT . It is essential to include the
SERIAL NUMBER of the Test Set.
SKT1
+30V
R18
SW1
OSC
O/P
COARSE
20V
R31
10V
C21
POLE CONTACT RELATIONSHIP
R32
RV33
SET
3150Hz
R35R34
7.7V
C22
VT11
VT12
SWITCH INDEX SHOWING
POLE
DEPRESSED RELEASED
R36
C23
C24
CONTACT
R37
16V
C25
R47
C32
VT16
12V3V
VT17
R48
C34
C33
R49
C35
drift
DRIFT
SENS
R55
SKT 20
set zero
RV56
VT8
7.5 - 9.4
(RV56)
20V
C39
MR4
8V
R50
R52
C36
R51
1 2 3 4 5 6 7 8 9 10 1112 13
+30V
MR3
R53
C37
C38
MR5
MR6
MR7
RV54
C40
R57
R58
R59
R211
R70
R60
C41
VT19
R61
R62
2V
0.4V
R63
VT20
R64
R65
13.5V
1.4V
30V
R66
C42
MR8
R67
R68
MR9
SKT 30
SKT 31
C43
C44
RV69
peak wow
cal (0.3%
range)
scope
meter
20V20V
C45
20V
L1
C26
R39
R38
C27
10.5V
VT13
R40
C28
R41
11V
VT14
R42
C30
SW 20
R43
C20
VT15
R44
R45
C31
6V
MR1
M1
- +
20V
R46
8.5V
MR2
27V
R17
R2
12V
VT2
26.4V
R3
C2
TH1
R6
R7
C4
VT3
14.6V
14V
C3
R5
O/P
RV19
R8
C5
1 2 3 4 5 6 7 8 9 10 1112 13
R9
R10
C6C7
FINE
R1
VT1
R4
C1
R11
R12
R13
R14
R15
R16
C8C9C10C11
R102
RV101
SET W&F
CAL
C63
100%
R103
RV 111
set
C61
VT31
R112
RV20a
R104
R113
R115
FREQ.
30V (onCAL)
R105
C62
VT32
R114
5.2V
C65
R116
RV20b
R106
MR21
R117
C64
MR22
R107
R108
R109
RV110
SET MV METER
CAL
14V
VT33
4.4V
R119
VT34
0.38V
R118
VT35
3.9V
RV121
R122
R120
SET
PHASE
BALANCE
6.1V
C66
C67
SKT 10
13
12
11
10
9
8
7
6
5
4
3
2
1
3.3V
6.8V
VT36
30V
R123
R124
R125
R126
R127
VT37
6.3V
14V
R128
C68
6.3V
FREQUENCY
X1 X10 X100 X1000
R81
BALANCE
C69
C81
R144
C83
R129
R143
R142
R141
SET
HF
C82
RV82
phase
SW15
C89
1mV
SW6a
100V
L.F.cut osc input
R83RV84a R85R86
C51
MR31
C84
C85
VT51
0.6V
R147
17V
R146
R145
C88
C87
C86
0.9V
0.6V
R151
RV152
mV meter
cal (1V range)
freq. coarse
R148
5.5V
R149
R150
VT52
W&F
drift
RV84bR88
R159
R158R157R156R155R154
C90
R153
12 POSN. SWITCH ONLY 6 TAGS
SHOWN. OPPOSITE TAGS LINKED
R160
C91
SW6b
DISTORTION
100% read
VT53
14V
C94
C93
R161
C92
RV87
freq. fine
13.9V
R162
VT55
VT54
R163
R166
R165
13.5V
1.6V
R164
CALMILLIVOLTMETER
RV87b
MR32
MR33
20V
1V
R167
1 2 3 4 5 6 7 8 9 10 1112 13
R169
MR34
R168
C100
C97
C98
C99
C95
C96
SW25
WOW & FLUTTER
drift 1% 0.3% 0.1%
+30V
SKT 11
C101
R174
R171R170
VT57
3.4V
1.4V
VT56
R175
0.8V
R173
C102
R172
MR35
+30V
C121
R176
C103
R212
R193
VT71
RV192
25VSET
30V
R191
P5 E
L N
R194
MR51
24.4V
NEUTRAL
LIVE
R195
VT72
VT73
C122
R196
FS1
C123
SUPPLY
ON
SKT 32
MR52
SW10
oscillator
LP1
FERROGRAPH
RECORDER TEST SET
RTS2
Serial No. 4515 onwards
CIRCUIT DIAGRAM
250-042 Issue 5
240
T1
VS1
220
117
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