NXP BUJ, PHx User Manual

NXP high voltage power bipolar transistors BUJ & PHx series
High voltage power bipolar transistors for lighting
Our high voltage power bipolar transistors are part of our industry-leading portfolio for energy-efficient lighting. Designed to support electronic ballast and transformer applications, they are available in versions from 700 to 1200 V and deliver very high efficiency with exceptional reliability.
Key Features
} Planar technology
- Market benchmark process technology
- Best cost-performance ratio of all technologies } High voltage capability
- V
- Suitable for push-pull topologies } Fast switching and low V
- Low fall time (tf) at turn-off reduces switching loss
- Low saturation voltage (V } Well-controlled h
- hFE distribution is well controlled by design and
- Tight parameter control reduces the need for banding or
- Design-in to customers’ circuits is easy
- Design-in for life – extended reliability } Integrated diode versions
- Reduced component count
- Simpler circuits
- Improved performance and reliability
up to 1200 V
CESM
production
selection
CEsat
) reduces conduction loss
CEsat
FE
Key Benefits
} Competitive and customer-oriented product portfolio } Experienced development team with deep understanding
on device physics
} Excellent application know-how and instant technical
support
} Well-controlled manufacturing and robust supply chain
The NXP BUJ and PHx series of high voltage power bipolar transistors use planar technology that delivers industry-leading cost-performance ratios. The high-voltage (up to 1200 V) capability is suitable for push-pull technologies. Fast switching times and low V combine to reduce switching and conduction losses. The well-controlled h for banding or selection, making design-in easier and extending reliability. Versions with integrated diodes reduce component count and simplify the design even further.
parameter reduces the need
FE
CEsat
ratings
How to design the base drive
BUJD103AD
Package Identifier:
- =TO220AB (SOT78) X = SOT186A B = D
2
PAK (SOT404)
D = DPAK (SOT428) R = TO92 (SOT54) reverse
pinning
Type Number
D = Transistor + internal
diode
PHE13003C
Package Identifier:
A = 1 Amp series in TO92 (SOT54) C = 1.5 Amp series in TO92 (SOT54) X = SOT186A
- = TO220AB (SOT78)
Type Number
E
transistor D = Transistor + internal diode
Current
Range:
3 = 1.0 – 2.0 Amp 5 = 4 Amp 7 = 8 Amp 9 =12 Amp
D = DPAK (SOT428)
Figure 1 shows a typical CFL drive circuit. Minimum power loss can be achieved by choosing the optimum base drive for the high voltage transistors.
Figure 2 shows power loss as a function of base drive. Weak base drive (too low a base current) causes too high a saturation voltage (V
), which results in higher than necessary
CEsat
conduction loss. Strong base drive (too high a base current) causes too much stored charge in the transistor when it’s in the on-state. As long as the transistor is conducting, that’s not a problem, but when the transistor has to be turned off, the excess charge that needs to be removed from the base can cause a longer fall time and higher switching losses. The base drive is normally optimized for a ‘typical’ transistor – that is, a transistor from normal production with a typical gain (hFE).
Figure 1. Typical CFL drive circuit.
Figure 2. Power loss as a function of base drive.
Figure 3 shows how turn-off I
affects the switching loss.
b
All charge stored in the junction when the transistor is conducting should be removed again at turn-off. Apply a negative base current to ensure quick turn-off. The time needed to remove the base collector charge is called the storage time and depends on the amount of negative bias applied to the base during turn-off. The storage time directly influences the circuit’s oscillating frequency. That is, a longer storage time leads to a longer delay and a lower frequency. As a result, transistor storage time plays an integral role in final circuit optimization.
Figure 3. Effect of base drive on switching loss.
The influence of gain on power loss
The production spread of high voltage transistors causes some variation in their gain h
(this variation is already very
FE
low for NXP transistors). As the gain has a direct effect on the optimal base drive for an individual transistor, a deviation from the typical gain value can cause the circuit to operate below its optimal point. This can be resolved by adjusting the base drive for every transistor in every individual TL ballast or CFL, but in a production environment this is normally not a feasible solution.
Figure 4. Power loss as a function of gain
The following is a recommended strategy for optimizing base drive for a given transistor. First, select typical transistors (that is, with a typical hFE) and observe their operation.
} If the lamp goes off or flickers at minimum supply voltage
(e.g. 150 V for a 230 V circuit), the oscillator is probably stalling. Increase the base drive.
by artificial adjustment of the production process.) With typical transistors, however, testing with high and low gain transistors is not as critical as the initial optimization. Any further changes to the base drive are usually minor, if needed at all. Once the
} If, when mains power is removed, the lamp extinguishes but
tries to restart a few times, resulting in flickering, then the oscillator is probably stalling prematurely, before the DC rail
circuit has been optimized for an NXP transistor, any individual transistor of the same type, with any h problems in the application.
voltage has reduced to zero. Increase the base drive.
Complete portfolio
} If, at minimum supply voltage, the transistor temperature rise
increases dramatically (possibly heading toward thermal runaway), and is often accompanied by premature turn-on of the transistors and very high turn-on losses, then the transistor turn-off drive is probably too weak. Increase the base drive.
NXP supports all the leading applications for energy-efficient lighting, including CFL, HID igniters, HF-TL, electronic transformers for low-voltage lighting, and dimmers. We specialize in best-in-class efficiency and low-power discrete solutions. In addition to the high voltage transistors, we offer best-in-class PFC diodes, SCRs, and triacs.
Once the base drive has been adjusted, recheck for acceptable operation and temperature rise at maximum supply voltage. Once operation at low voltage has been optimized, acceptable operation at high voltage usually follows.
Customer focus
NXP offers a roadmap of continuous process development and customer-driven innovation. Our experienced development teams have a deep knowledge and experience of bipolar
If high and low gain transistor samples are available, the above tests can be repeated for further fine tuning of the base drive. (Note that high and low gain limit samples are not possible with NXP standard production, due to the tight process control. These samples are only available at initial product development, when high and low gain samples are “forced”
technology, and we have specialists who proactively discuss technical details with customers. We offer complete testing capabilities at our application labs, located in Europe and China. Furthermore, our well-controlled manufacturing processes and robust supply chain make us a trusted partner for quality, support and lead time.
High Voltage Power Bipolar Transistors for lighting, SMPS and industrial applications
V
CESM
(V)
700
1000 5 145 2.5 12 3 BUJ303A
1050 5 200 2.5 10.5 3 BUJ303B
120 0 6 17 0 2.5 15.5 3 BUJ403A
* Integrated diode
Types in bold red represent new products Package drawings are not to scale
I
(max)
C(DC)
(A)
1 80 1 7. 5 0.8 BUJ10 0LR
1 80 1 7. 5 0.8 PHE130 03A
1 50 1 14 0.75 BUJ100
1.5 100 0.5 9 1 PHE13003C
1.5 100 0.5 9 1 PHD13003C*
4 30 2 12.5 3 BUJ103 A BUJ103 AX BUJ103 AD
4 30 2 12.5 3 BUJD103AD*
4 100 2 17 2 PHE130 05 PHE130 05X
4 100 2 17 2 PHD13005* PHD13005D*
8 20 5 11 4 BUJ105A BUJ105AB BUJ105AD
8 20 5 11 4 BUJD105AD*
8 40 5 9 5 P HE130 07
10 20 5 11 6 BUJ10 6A
12 100 5 6min - 30 max 8 PHE13 009
ind. t
25
(ns)
f
o
C
(typ)
@ I
(A)
C
hFE (typ) @ I
(A)
C
SOT54 (TO92)
BUJ series part numbering
FE
SOT78
(TO220AB)
SOT 186A
(isolated
TO220AB)
PHx series part numbering
will operate without
SOT404 (D2PAK )
SOT428
(DPAK )
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