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AN3400 Datasheet(PDF) 7 Page - STMicroelectronics

Part # AN3400
Description  Analysis and simulation of a BJT complementary pair in a self-oscillating CFL solution
PDF  78 Pages
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Manufacturer  STMICROELECTRONICS [STMicroelectronics]
Direct Link  http://www.st.com
Logo STMICROELECTRONICS - STMicroelectronics

AN3400 Datasheet(HTML) 7 Page - STMicroelectronics

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AN3400
Circuit description
Doc ID 018840 Rev 1
7/78
working frequency and, consequently, the lamp power are influenced by the sizing of both
L1 and C2 components. Capacitor C2 has also the function of putting the base current in
phase with the collector current. Resistance R2 of the series R-C network has the function
of regulating the current level to provide to the bases of both transistors acting on the power
lamp. In the proposed driving solution, the two capacitors C3 and C4 are charged with
opposite polarity to each other and assuming the same polarity of the base-emitter voltage
of the relevant bipolar transistor. In the regular functionality, when a capacitor goes through
a charging phase, before or during the conduction time of the relevant bipolar, so the
opposite capacitor is discharging contemporarily with a long constant time due to the series
with the breakdown resistance R4. So, this resistance R4, inserted between the bases of
the two transistors, creating an alternative path for the discharge of each capacitor, also
avoids that the oscillation is blocked during startup phase when one of the two capacitors is
fully charged. Regulating the discharge time of each capacitor, this resistance allows to fine
tune the working frequency and consequently the power supplied to the lamp. Two
capacitors C3 and C4 are not totally discharged during a forcing voltage source period but
maintain always a residual charge passing from the discharging to the charging transient.
Therefore, current across the breakdown resistance R4 flows always in the same direction
going from the PNP to the NPN base because the two capacitors maintain always the same
polarity during a period of the voltage signal across the C2 filter capacitor. A breakdown
resistance with a too high value can increase the working frequency but also can bring the
reverse biased base-emitter junction of the inactive device in breakdown condition. And vice
versa, a too low value of the breakdown resistance could cause re-conduction peaks in the
PNP transistor at the high temperature when the emitter-collector voltage reaches the
maximum value. In particular only the PNP device can show the phenomena above
mentioned because it has a lower base-emitter breakdown voltage and it has a higher low
current hfe than the NPN one. Setting the resistance R4 in order to guarantee a VBEoff value
in the range -4 V to -7 V, it is possible to avoid breakdown phenomena for the base-emitter
junctions of the bipolars and, at the same time, anomalous re-conduction effects due to
unexpected disturbances.



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