📄 12v flourescent lamp inverter.htm
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<P>Fluorescent tubes use far less energy than incandescent lamps and
fluorescent tubes last a great deal longer as well. Other advantages are
diffuse, glare-free lighting and low heat output. </P>
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<DIV class=wpcaption>Fig.1: two switch-mode circuits are involved here:
the DC-DC inverter involving IC1, Q1 & Q2 and the fluoro tube driver
which converts high voltage DC to AC via IC3 and Q3 & Q4 in a
totem-pole circuit.</DIV></DIV>
<P>For these reasons, fluorescent lighting is the natural choice in
commercial and retail buildings, workshops and factories. For
battery-powered lighting, fluorescent lights are also the first choice
because of their high efficiency.</P>
<P>The main drawback with running fluorescent lights from battery power is
that an inverter is required to drive the tubes. Inverter efficiency then
becomes the major issue.</P>
<P>There are many commercial 12V-operated fluorescent lamps available
which use 15W and 20W tubes. However, it is rare to see one which drives
them to full brilliance. For example, a typical commercial dual 20W
fluorescent lamp operating from 12V draws 980mA or 11.8W. Ignoring losses
in the fluorescent tube driver itself, it means that each tube is only
supplied with 5.9W of power which is considerably less than their 20W
rating. So while the lamps do use 20W tubes, the light output is well
below par.</P>
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<DIV class=breakoutTitle>Warning:</DIV>This circuit generates in
excess of 300V DC which could be lethal. Construction should only be
attempted by those experimenced with mains-level voltages and safety
procedures. </TD></TR></TBODY></TABLE>
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<P>Our new fluorescent inverter drives 36W or 40W tubes to full brilliance
and has the option to dim the tube down to about 80% brightness. So not
only do you get full brightness when you want it but you can dim the tube
down when full brightness is not required and you want to conserve power
drawn from the battery.</P>
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<DIV class=wpcaption>Fig.2: this is the internal schematic for IC1. The
TL494 switch-mode controller.</DIV></DIV>
<P>Built on a long thin PC board, the inverter fits easily into a standard
36/40W batten.</P>
<P>Drive for the fluorescent tube is controlled with a specialised IC
which provides filament preheating before the tube is ignited. Once the
tube is alight it monitors the tube current to maintain constant
brightness. This current feedback control also provides for the dimming
feature.</P>
<P>By the way, this project is quite similar in concept to the fluorescent
inverter described in the November 1993 issue of SILICON CHIP. This
earlier circuit is now superseded.</P>
<H3>Block diagram</H3>
<P>Fig.1 shows the general arrangement of the fluorescent inverter. The
12V supply is stepped up to 334VDC using IC1 & IC2, Mosfets Q1 &
Q2 and transformer T1.</P>
<P>IC1 is the well-known Texas Instruments TL494 pulse width modulation
controller. The internal functions of IC1 are shown in Fig.2. It contains
a sawtooth oscillator, two error amplifiers and a pulse width modulation
comparator. It also includes a dead-time control comparator, a 5V
reference and output control options for push-pull or single ended
operation.</P>
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<DIV class=wpcaption>Scope1: These two waveforms show the gate drive to Q3
and Q4 when the fluorescent tube is at full brightness. Top trace is the
gate drive to Q4, a nominal 12V peak-to-peak signal. Lower trace is the
gate drive to Q3, which is from 0-334V plus the gate voltage when switched
on. The small step in the top of the waveform is when the gate goes to 12V
above the 334V supply. </DIV></DIV>
<P>Oscillator components at pins 5 and 6 set the operating frequency and
for our circuit this is around 100kHz. This frequency was selected to
enable use of a relatively small toroidal core for the transformer. The
PWM controller generates variable width output pulses at pins 9 and 10, to
ultimately drive the gates of Mosfets Q1 and Q2 via the CMOS buffers in
IC2, a 4050 hex buffer package.</P>
<P>Mosfets Q1 and Q2 drive the centre-tapped primary winding of
transformer T1. The centre-tap of the transformer's primary winding
connects to the +12V supply while each side of the primary winding is
connected to a separate Mosfet. Each Mosfet is driven with a squarewave so
that when Q1 is on, Q2 is off and when Q2 is on Q1 is off.</P>
<P>With Q1 on, 12V is applied to the top half of the transformer primary
winding. Similarly, when Q2 turns on, 12V is also impressed across the
lower primary winding. The resulting square waveform on the primary is
then stepped up by the secondary winding. High speed diodes rectify the AC
output from the transformer T1, while a 470nF 630V capacitor (C4) filters
the output to provide a stable DC voltage.</P>
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<DIV class=wpcaption>Scope2: These waveforms are identical to those in
Scope1 except that now the frequency is much higher, at 65kHz, to dim the
fluorescent tube. Notice the "dead time" between Q4 being switched off to
Q3 switched on. This prevents high current pulses which would destroy the
Mosfets if both were on at the same time.</DIV></DIV>
<P>A portion of the DC voltage output (called the error voltage) is
returned to IC1 for feedback control and the pulse width modulation is
varied to maintain the 334V output.</P>
<P>The high voltage DC from the inverter is applied to the fluorescent
tube via Mosfets Q3 & Q4 and an LC network consisting of L2 and C1.
Mosfets Q3 & Q4 are switched alternately by the ballast driver IC3, an
L6574 fluorescent ballast driver, made by SGS-Thomson. The resulting
squarewave signal is applied through inductor L2 and capacitor C1 to the
fluorescent lamp. The inductor is included to provide AC current limiting
while capacitor C1 blocks DC current flow.</P>
<P>During the starting phase, Q3 and Q4 are driven at a very high
frequency and this provides a current flow through L2 and C1, the top tube
filament, through C2 and the lower tube filament and then to ground via
the current sense resistor R1. This current is limited to a low value by
the impedance of L2 and it heats up the lamp filaments so the tube start
easily. After about one second, the drive frequency is lowered to the
series resonant frequency of L2 and C2 and the resulting high voltage
across C2 fires the tube. Once the tube is fired, the drive frequency is
further reduced to provide full tube brightness.</P>
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<DIV class=wpcaption>Scope3. These are the gate drive signals to Q1 and Q2
when the fluorescent tube is driven to full brightness. Frequency is
around 100kHz. Note the "dead time" between one Mosfet turning off and the
second Mosfet turning on.</DIV></DIV>
<P>As you might expect, there is a fair amount of circuitry packed into
the ballast driver IC; its internal workings are shown in Fig.3. An
oscillator section comprises the VCO (voltage controlled oscillator) and
the current sources set by resistors Rign and Rpre at pins 4 and 2
respectively. Frequency during starting is controlled by resistor Rpre in
conjunction with capacitor CF at pin 3. This sets the maximum frequency.
Once the tube is started, the frequency is set by Rign and capacitor CF.
An op amp at pins 5, 6 & 7 can be used for frequency control.</P>
<P>The duration of the tube filament preheat is set by capacitor Cpre at
pin 1. The enable inputs at pins 8 & 9 can be used to reinitiate
starting if the tube does not fire or to shutdown the circuit if a tube is
not installed.</P>
<P>The gate drive for the Mosfets is interesting. Mosfet Q4 is driven
directly via the low voltage gate (LVG) driver at pin 11. When pin 11 goes
high, Q4 is switched on and when pin 11 is low, Q4 is off.</P>
<H3>High side switching</H3>
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<DIV class=wpcaption>Scope4: This waveform shows the firing cycle of the
fluorescent tube and is an attenuated signal of the actual tube voltage.
The voltage is initially high and then drops once the tube has
fired.</DIV></DIV>
<P>Mosfet Q3 requires a special gate driver to allow it to drive the high
voltage (HV) supply. The special gate driver comprises the bootstrap
diode, level shifter, high voltage driver (HVG) and capacitor Cboot
between the source of Q3 and Vboot. When Q4 is switched on, Q3 is off and
so capacitor Cboot can be charged from the supply at Vs via the bootstrap
diode and Q4 (to ground).</P>
<P>Thus Cboot will have the supply voltage across it. When Q4 is switched
off and Q3 is switched on, the entire gate drive section for Q3 is pulled
up to the HV supply and the gate drive is higher than this by the Vs
supply stored on Cboot. The gate drive circuit (HVG) thus maintains its
supply from Cboot. The bootstrap diode is now reverse biassed and plays no
further part in the operation. </P>
<P>When Q3 is switched off and Q4 is switched on, Cboot can be topped up
via the bootstrap diode again. The capacitor value needs to be
sufficiently large to prevent the HVG driver supply from drooping as it
needs to charge the gate capacitance of Q3. </P>
<H3>Circuit details</H3>
<DIV class=wpimg style="WIDTH: 302px"><A
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<DIV class=wpcaption>Fig.4: the full circuit of the fluorescent inverter.
IC3 is the clever component, varying the tube drive frequency between
100kHz and about 30kHz to preheat the filaments, ignite the tube and then
maintain the tube current at the correct value.</DIV></DIV>
<P>The full circuit of the fluorescent inverter is shown in Fig.4. IC1 is
the TL494 PWM controller. Its frequency of operation set at around 100kHz
by the 4.7kW resistor and 1nF capacitor at pins 6 and 5 respectively. </P>
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