Die Bewertung des Threads entspricht der besten Post-Bewertung. Haben Sie schon einen Post hier bewertet?

Tube Tester AVO V.C.M. 163 – Measurement Principle (revised)

Martin Renz Ernst Erb Vincent de Franco Martin Bösch Mark Hippenstiel Bernhard Nagel Otmar Jung Heribert Jung Eilert Menke 
Bitte klicken Sie ganz oben rechts das blaue Info-Zeichen, um Instruktionen/Hilfe zu erhalten.
Forum » Apparate: Physik - Radios - bis TV » MODELLE IM RADIOMUSEUM » Tube Tester AVO V.C.M. 163 – Measurement Principle (revised)
Kurt Schmid
Kurt Schmid
D  Beiträge: 66
Schema: 3
Bilder: 3
23.Mar.12 09:49
Anzahl Danke: 22
Antworten  |  Sie sind nicht eingeloggt (Gast).   1

Tube Tester AVO V.C.M. 163 – Measurement principle of plate/screen current and mutual conductance

by Kurt Schmid (DH3PJ) Mainz, Germany


The AVO VCM 163 is one of the few tube testers (British: valve tester) being able to measure tube electrode currents, e.g. plate and screen current (fig. 1, left-hand meter movement) as well as mutual conductance (fig. 1, right-hand meter movement) simultaneously. The VCM 163 is the latest and most elaborate tube tester ever built by AVO.

Figure 1:    The AVO Valve Characteristic Meter V.C.M. 163

All voltages applied to the electron tube under test are pure 50 Hz line frequency sine waves. The plate (British: anode) as well as the screen electrode via diodes D1 and D2 are supplied with sinusoidal positive half wave voltages (cf. fig. 2).  AVO unusually terms rectifier diodes D1 and D2 ‘suppressor’ diodes probably due to the fact that they suppress the negative half wave.  Via diode D4 an unsmoothed negative half wave (grid BIAS) is applied to the grid electrode in proper phase relationship, i.e. anti-phase, to the positive electrode voltages. This is quite a clever and economical principle because the power supply becomes extremely simple (among other things no filtering). In addition power requirement of the line transformer (C core type) is half compared to a DC supply.

A)     Principle of measurement of plate and screen current

AVO engineers have evaluated and verified that if alternating electrode voltages are applied in their correct proportions an amplifying tube (by virtue of its property of self-rectification) produces DC plate and screen currents, which for all practical purposes, bear an almost constant relationship to those obtained from its DC static characteristics. In the VCM 163 the following relationship between AC supply and DC static characteristics is implemented:

The left meter movement (cf. fig. 1) reads DC plate and screen current continuously. As a further consequence of the fictive static characteristic of the VCM 163 test conditions of a tube can be directly obtained from the tube manufacturers published curves or data.

B)     Principle of mutual conductance measurement  

Measurement of mutual conductance (= transconductance) is based on a sophisticated operational principle using a transistorized high frequency (HF) oscillator and a frequency selective HF amplifier (fig. 2, High Pass Filter & Amplifier). The grid BIAS signal and the HF signal are added and routed to the grid of the test tube. Detailed schematics are shown in figs 7 & 8.

Figure 2:     Basic circuit for mutual conductance measurement
                    (Source: Operational Manual)

Below, a few voltage measurements performed to clarify the principle of mutual conductance measurement as used in this premium instrument developed by AVO are presented.

The amplitude of the negative 50 Hz grid BIAS voltage can be selected in four ranges from 0-100 Volt. This BIAS voltage is superimposed by a low voltage grid HF signal the amplitude of which is well stabilized. HF modulation of the grid voltage results in a proportional plate HF current. Mutual conductance is derived from the band-pass filtered plate HF current set into relation to the applied grid HF signal amplitude.

The following voltage measurements were registered using a Tektronix TDS 210 oscilloscope. There was no test tube inserted into the VCM 163.

Due to the fact that the high frequency grid signal is magnitudes smaller than the Ugrid BIAS amplitude the superimposed grid signal is not readily visible (figure 3).

Figure 3:     Simultaneous display of Uplate and Ugrid (50 Hz frequency)

Channel 1:  positive half wave plate voltage (Uplate) at 50V/div
Channel 2:  negative half wave grid voltage (Ugrid) at 5V/div

To visualize the grid HF signal ‘riding’ on the 50 Hz grid BIAS supply amplification was increased from 5 Volt to 0.2 Volt per division.

Figure 4:     Ugrid at higher amplification (200mV/div)

Especially in the horizontal parts of Ugrid recording the superimposed HF grid signal now becomes noticeable as wide traces (fig. 4, arrow). For further clarification of the combined signal to the grid figure 5 illustrates the grid HF signal component using higher amplification (20mV/div) and faster time deflection (50µs/div).

Figure 5:     Grid signal (Range 0-6 mA/V)

Left insert:      Grid HF signal at the rising part of the 50Hz BIAS sine wave
Right insert:    Grid HF signal at zero BIAS voltage

Frequency of the grid HF signal (not mentioned in any AVO manual) was found to be 14.68 kHz.

The AVO VCM 163 offers three selectable ranges for mutual conductance measurement by switching the amplitude of the grid HF signal.

Figure 6:     Grid HF signals at 3 selectable mutual conductance ranges
Voltages shown in the MEASURE panel (right-hand side) correspond
to the 0-6 mA/V range

Tubes with low mutual conductance (0-6 mA/V) are measured using a large amplitude grid HF signal whereas tubes with high (0-20 mA/V) or very high mutual conductance (0-60 mA/V) require lower signal amplitudes.

As a general purpose tube tester the VCM 163 in addition to the above described features is able to:

•    check the heater continuity
•    measure insulation  between electrodes with the tube either being cold or hot
•    check rectifiers and diodes under load conditions
•    measure gas current up to 100 µA f.s.d.

A remarkable highlight of the mechanical sturdy construction of the instrument is the use of a huge thumbwheel switch 13 pin electrode selector (cf. fig. 1).

Figure 7:     Circuit diagram of the AVO VCM 163

Figure 8:     Circuit diagrams of the transistorized modules (shown as block diagrams in fig. 7)

Dieser Beitrag wurde am 30.Mar.12 08:24 von Kurt Schmid editiert.

Michael Watterson
IRL  Beiträge: 967
Schema: 650
Bilder: 2496
15.Apr.12 01:51

Anzahl Danke: 14
Antworten  |  Sie sind nicht eingeloggt (Gast).   2

So actually if an external meter is put in series with a Top Cap Anode lead (or at the link intended for magic eye Anode loads) the measured current will be 1/2 the current indicated on the left meter.

Similarly if you measure the Anode voltage with a DMM externally, it will be lower than the voltage indicated on the dial.

Kurt Schmid
Kurt Schmid
D  Beiträge: 66
Schema: 3
Bilder: 3
15.Apr.12 02:47

Anzahl Danke: 18
Antworten  |  Sie sind nicht eingeloggt (Gast).   3

Michael Watterson wrote: 'Similarly if you measure the Anode voltage with a DMM externally, it will be lower than the voltage indicated on the dial.'


The AVO VCM 163 service manual shows a table for DC (!) voltage checks for anode and screen voltages:

Nominal voltage indicated [VDC] Actual electrode voltage [VDC]
100 51,5
200 102.3
400 204

On my VCM 163 I could confirm these DC values. Using a somewhat special True RMS Voltmeter (UT803) that's able to measure DC, true RMS, true RMS + DC:

100 50,8 61,3 79,2
200 101,5 123 158,7
400 204,1 245,3 316,7

Results confirm the assumptions of AVO as shown in section A)


The above results already have been postet at: