Before 1960 or so, opto-electronic instruments and devices employed vacuum tubes. Here we describe a regulated variable high voltage power supply that finds general use in the restoration of vintage laboratory equipment as well as at the experimenter’s workbench. The supply is based on earlier work by Leigh Bassett1 and Cam Hartford2. A goal was to make use of the previous work and to create a printed circuit board (PCB) that could be used by many builders for unique applications. To demonstrate performance and to encourage readers to build something useful, a battery of tests were performed on the PCB and I breadboarded a two-channel preamp using two 6SN7 vacuum tubes. As we’ll see at the end of this note, the bare PCB is available from the Antique Wireless Association AWA) (http://www.antiquewireless.org).
Consider the schematic shown in Fig. 1. The circuit utilizes the LR8N high voltage regulator and the TIP50 pass transistor in the configuration of Bassett and Hartford. AC input to E1/E2 is supplied by a suitable isolation transformer. Alternatively, for use in existing DC circuits, DC voltage can be applied at E8. Input voltage should not exceed 265 VAC or 375 VDC.
Variable resistor, VR1, is used to select the output DC voltage at E6 and can be mounted on the board or remotely on a chassis using E4 and E5. If a fixed output voltage is desired, R4 and VR1 can be omitted and R2 can be used in conjunction with R1.
The TIP50 resides on a suitable heat sink, which can be mounted on the PCB or remotely. When mounted properly on the PCB, the heat sink is at B- potential. There is also a provision to “run barefoot” for very low current applications using connection point E9, which is the low-current output of the regulator. B- is at E7, and is isolated from chassis ground to allow for a floating power supply. The circuit also allows the use of a center-tapped power transformer using E1/E2 and E3 for the center tap. In this configuration, D1 and D2 are omitted.
While the circuit in Fig. 1 is quite general, a representative case with the following requirements and components is considered:
Voltage, Output: 90-330V DC, variable
Voltage, Input: 120V AC
C1: 100μF 450V electrolytic capacitor
C2: 1μF 450V electrolytic capacitor
C3: 22uF 450V electrolytic capacitor
D1-D5: 1N4007 diode
HS1: Depends on user requirements, Ohmite FA-T220-38E fits on PCB
PCB: AWA Rev 6, 8/2020
Q1: TIP50 NPN power transistor
Q1 Mounting Kit: AAVID 4880MG
R1: 2k, 1/4-watt resistor, 1%
R2: Used for fixed output voltage only; not used with VR1
R3: 150k, 2-watt, 5%
R4: 130k, 1/4-watt resistor, 5%
T1: Power transformer, Triad VPS230-110
U1: LR8N3-G 3-terminal adjustable regulator
VR1: 500k 1/2-watt, Bourns 3296Y-1-504LF
It is important to note that the TIP50 transistor will get hot at relatively low output voltage and high output current, and heat sinking is required. The power dissipation in the TIP50 is given by Vce*Ic. In our example, the unregulated DC voltage will be about 365V DC depending on the input AC voltage. For illustrative purposes, at an output voltage of 265V DC and ambient temperature of 25°C, the maximum power dissipation, Pd-max, for the TIP50 is given by
where Rjc is 3.125 °C/W and HSrth is about 10.4 °C/W for the Ohmite FA-T220-38E (measured to be much higher than the specification of 3.8 °C/W). Using these values,
If Vce=365V-265V=100V and Pd-max=9.24 watts, then the maximum load current, Ic-max=92.4ma. This is just an illustrative calculation and the actual allowable values depend on the specific heat sink being used, operational duty cycle, safety margin, and unobstructed air flow. Some thought must be given to power dissipation in cases where the PCB, with on-board TIP50, is mounted in a location where cooling is compromised.
The minimum input-output voltage differential across the LR8N should be greater than about 20v. The following table gives an approximation of output voltage as a function of R2, given R1=2k, using 1% resistors (in this explanation, R4 and VR1 are not used.)
Figure 3 shows the LR8N PCB energizing a two-channel vacuum tube line stage. Barbour and Kittleson3 gave a schematic and a detailed description, which allowed the build to be completed in an afternoon using a repurposed chassis. It operates at B+=320V DC, gain is 15 and essentially flat from <10Hz to >100KHz and it’s plenty to drive most any tube or solid state amplifier. The PCB really streamlined the process and gave regulated B+ as a nice benefit.
The LR8N PCB was created to be used in a wide variety of user-specific applications. I’ve used the circuit widely in buffers, pulse generators, signal generators, oscillators, amplifiers, HV triggers/shutters, differential amplifiers and active filters. It comes in handy when rebuilding vintage electro-optic instruments and devices.
Speaking of the older equipment that shaped the future, please do not scrap it. Too much of our optics heritage has been landfilled already. Please send me an email about it (dci at perluma dot com) and consider donating it for study and preservation.
As mentioned earlier, a professional quality, silk-screened circuit board is available (High Voltage Power Supply PCB) and it ships with a schematic and representative parts list. Their website will soon include test results using several different power transformers with this PCB.
There is a long-standing commitment to supporting builders of vacuum tube audio amplifiers, HiFi equipment as well as restorers of vintage test equipment and amateur radio gear. I’m trying to highlight the need for a similar commitment to help preserve our optics heritage.
1. Leigh Bassett, “A solid-state filter choke or field coil replacement,” edited by Ken Owens, AWA Old Timers Bulletin, 45-2-14, 2004.
2. Cam Hartford, “A Power Supply for April’s Two-Tube Transmitter,” CQ Magazine Digital Edition, June 2011.
3. Eric Barbour and Charles Kittleson, “VTV Octal Line Stage Project,” Vacuum Tube Valley, Issue 11, p. 10, Spring 1999.