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ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING
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Lamp UMZCH entry-level (work on the bugs). Encyclopedia of radio electronics and electrical engineering

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Encyclopedia of radio electronics and electrical engineering / Tube Power Amplifiers

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The time that has passed since the assembly of the first working UMZCH layout has shown once again that, in principle, there is no such design that could not be improved. If for each change in the circuit it was necessary to manufacture a new amplifier, then at least half of the city's population would be "happy" with them. However, this is hyperbole :-)

In reality, several changes in the scheme were tested, contributing to the "more correct" use of lamps, but without requiring significant alteration of the design.

Schematic diagram one channel of the modified amplifier is shown in fig. one

Lamp UMZCH entry-level (work on the bugs). Scheme of the modified UMZCH
Rice. 1 (click to enlarge)

The newly introduced elements first of all violated their usual numbering on the circuit diagram, so be careful - hereinafter the new numbering will be used.

About the scheme

First of all, on the strong recommendation of real audiophiles, capacitors were introduced into the auto-bias cathode circuits: C4 and C7 for the VL1 and VL2 tubes, respectively. Thanks to these capacitors, the influence of cathode resistors is eliminated (in fact, local current feedback is eliminated) on the output resistance of the amplifier stages (without these capacitors, it is noticeably higher). And, if for the cascade on VL1 this is not so obvious, then the introduction of the capacitor C7 into the cathode circuit of the output pentode VL2 made it possible (albeit quite a bit) to increase the maximum output power of the amplifier.

The chain of supplying the general OOS (R4, R7) to the cathode circuit of the first lamp (R5, C4) is somewhat complicated. This was done in connection with the desire to reduce the influence of the parameters of this chain on the VL1 lamp mode. Now the bias voltage of the VL1 lamp is almost completely determined by the resistance value of the cathode resistor R5, as a result of which there is no need to select it after changing the feedback depth.

Another two-position jumper JP2 has been introduced, which increases the degree of convenience for those who like to experiment. The jumper allows you to switch the output lamp from pentode mode to triode mode and vice versa. (The diagram shows a pentode connection - when the screening grid is connected to a power source. In a triode connection, the screening grid is connected directly to the anode, which ensures a sufficiently deep local voltage feedback, while the current-voltage characteristics - I-V characteristics - lamps become very similar to I-V characteristics of triodes , which is why such a name arose.) It should be noted that the use of this feature requires special care from the experimenter - changing the lamp mode often leads to the need to correct the offset value on the first grid, which means that it is also necessary to change the value resistance R10.

Printed circuit board has been updated to reflect the above changes. It was possible to keep its former size and mechanical parameters. But since the installation has become denser, when assembling, you need to pay attention to the dimensions of the electrolytic capacitors used.

The printed circuit board version with the JP2 jumper, however, does not seem to be entirely successful due to the excessive number of additional conductors, which significantly increase the mounting density (the voltage between the jumper contacts can reach 300 Volts - therefore, you need to be careful about observing the gap between the tracks of the board to avoid breakdown).

PCB with JP2 [gif, 300dpi, 122 kb]
PCB without JP2 [gif, 300dpi, 119 kb]

About heating capacitors

Many have noticed that during the operation of the amplifier, the electrolytic capacitors heat up. Heating occurs due to the thermal radiation of the lamps and, in my opinion, is not at all dangerous - capacitors C3 and C6 heat up to a temperature of about 40-45 degrees, and this is very little. However, it should be noted that the layout of the printed circuit board of the amplifier is designed for an open design and, if the amplifier mounted on the proposed printed circuit board is placed in any case, it is possible that heat shields will have to be used to reduce the degree of heating of the capacitors.

About replacing lamps

The closest in parameters to the 6P14P lamp is 6P18P. In fact, the lamps are very close (in the absence of markings, they cannot be distinguished at all) and differ only, according to the reference book, in the nominal voltage at the anode, which for 6P18P is 170 V at the maximum allowable 250 V. However, 6P18P works fine even at higher voltages and can be installed instead of 6P14P without any changes in the circuit. Unfortunately, this is where the list of lamps suitable for such a replacement ends - for the rest of the lamps, the selection of a cathode resistor is necessary. The closest parameters to 6P14P lamps:

Lamp Anode current Bias R10 Resistor power output power
6P15P 35 mA -2.5 B 75 ohm 0.5 W 2.5 W
6P33P 48 mA -15 B 270 ohm 2 W 4.2 W

It is possible to use a 6P1P lamp (with a 240 ohm cathode resistor), but it has a different pinout, which entails the need to change the printed circuit board pattern. It is difficult to use a 6P43P lamp (although the pinout is the same) due to the large value of the bias required for its operation (for this lamp it is more profitable to use the so-called fixed bias from a separate source).

Lamp 6N3P without any alterations is replaced by a lamp 6N26P. Without changing the circuit, it is possible to use 6N1P, but it differs in the pinout. 6N2P and 6N23P are of little use due to the low anode current of 6N2P (only 2,3 mA) and the strong microphone effect of 6N23P, but you can try to use them, also taking into account their pinout (similar to pinout 6N1P) /

Author: Andrey Kovalev, Tyumen; Publication: cxem.net

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