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4

UVtron DRIVE CIRCUIT

Operating a UVTRON requires a high voltage of about 350 V. Figure 4 shows the basic circuit for the DC-DC con-

verter high-voltage power supply and the operating waveforms for each part. In this case, it is important to lower the 
converter oscillation frequency, f, to reduce the capacitance of capacitor C

1

 for smoothing the rectified high voltage, and 

to raise the power supply output impedance. Here is an explanation of the operation of this circuit. (See Figures 4-1 and 
4-2.)

Point (a):

  This is the converter oscillation waveform. Pulses with a width of a few microseconds are generated at in-

tervals of a few milliseconds to a few tens of milliseconds.

Point (b):

 The height of pulses is raised in proportion to the winding ratio for the step-up transformer.

Point (c)

:  High DC voltage Ebb is supplied to the UVTRON's anode by rectifier diode D and smoothing capacitor C

1

.

Point (d):

 Discharge starts when ultraviolet light enters the UVTRON. The charge on C

1

 begins to flow as discharge 

current, i, to generate narrow voltage pulses across R and C

2

.

Point (e):

  The charge on C

is exhausted, the anode voltage falls below the discharge sustaining voltage Vs, and the 

discharge stops. The anode voltage does not recover until the next charge. During that period, the ions in 
the UVTRON are quenched. 

Point (f):

  If no ultraviolet light enters the UVTRON, the anode voltage recovers to Ebb, and there is no discharge un-

til ultraviolet light is received.

The UVTRON repeats this cycle to indicate the presence or absence of ultraviolet light with pulse signal output. 

Here, it is important that the converter oscillation interval (l /the oscillation frequency f) be greater than the time re-
quired for the ions generated in the UVTRON tube by the discharge to be quenched, so this interval must be from 5 to l0 
milliseconds. This period is called the quenching time. Also, since the capacitance of smoothing capacitor C

1

 influences 

the discharge current, it is best to reduce the capacitance of C

1

 in order to retard the wear on the electrodes and to reduce 

the number of ions generated. The optimum capacitance is a few tens of picofarads.

i

+

V

1

D

Tr

C

1

C

2

R

UV TRON

A

UV

K

(a)

(c)

(b)

(d)

TPT C0011EA

TPT C0011EA

UVTRON OUTPUT 

WAVEFORM

OSCILLATION 

WAVEFORM

OSCILLATOR 

CIRCUIT

UVtron Drive Circuit

Figure 4-1: UVTRON Drive Circuit

Содержание UVTRON

Страница 1: ...TECHNICAL INFORMATION How to Use UVTRON...

Страница 2: ...ensity of a gas burner flame city gas tungsten lamp and the sunlight on the earth s surface along with UVTRON spectral response characteristics As this figure shows the UVTRON has no sensitivity in th...

Страница 3: ...Meanwhile the positive ions are accelerated towards the cathode and the resulting collisions with the cathode generate a great number of secondary electrons As this cycle is repeated a large current...

Страница 4: ...R and C2 Point e The charge on C1 is exhausted the anode voltage falls below the discharge sustaining voltage Vs and the discharge stops The anode voltage does not recover until the next charge Durin...

Страница 5: ...next point that must be considered is the background BG The BG is caused by sporadic discharges that occur due to radiation such as cosmic rays and static electricity even if no ultraviolet light ent...

Страница 6: ...is generated to the output circuit and the counter is reset Point d At the output circuit the output pulses from the counter are lengthened to the necessary time interval T2 and are output 1 Figure 8...

Страница 7: ...igure 8 Operation Time Chart for Signal Processing Circuit SUPPLY VOLTAGE AND SENSITIVITY Figure 9 shows a typical relation between the supply voltage and the UVTRON sensitivity The UVTRON is more sen...

Страница 8: ...nterfere with each other optically 2 Humidity Humidity around the UVTRON leads may cause leak current dropping the anode voltage and stopping the UVTRON from operating In particular if dirt or dust ge...

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