Characteristics and principle of PT4107_DB03 full voltage 20W fluorescent lamp switch constant current source

Publisher:忠正Latest update time:2012-01-14 Source: 电子发烧友Keywords:PT4107_DB03 Reading articles on mobile phones Scan QR code
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Basic features

AC non-isolated high-frequency switch buck constant current mode
AC 85~245V, 50~60Hz working range
Series charging, parallel discharge passive power factor correction
Can be installed inside a 28mm lamp tube
Working environment temperature 0~75oC
meets IEC61000-3-2:2001 requirements

Circuit diagram and actual photos

The circuit is shown in Figure 1. The AC mains inlet is connected to a 1A fuse FS1 and an anti-surge negative temperature coefficient thermistor NTC. After that is the EMI filter, which consists of L1, L2 and CX1. BD1 is a rectifier full bridge with 4 high-voltage silicon diodes inside. C1, C2, R1, D1~D3 form a passive power factor correction. The working principle can be found in our company's article "Optimization Method for Designing LED Fluorescent Lamps Using PT4107". The PWM control chip U1 and the power MOS tube Q1, ballast inductor L3, and freewheeling diode D5 form a Buck step-down conversion. U1 collects the peak current on the sensing resistor R6~R9, and the internal logic controls the pulse duty cycle of the GATE pin signal for constant current control. The chip is powered by an electronic filter composed of T1, D4, C4, R2~R4 after stepping down. This filter has a high internal resistance and a small output impedance. It can provide a stable voltage of about 16V to ensure that the chip works stably in the full voltage range. R5 is part of the chip oscillation circuit, changing it will adjust the oscillation frequency. The potentiometer RT is not used to dim the light in this circuit, but to fine-tune the current of the constant current source so that the circuit reaches the designed power. The parameters of this circuit are designed for 22 LEDs in series, 15 in parallel, and driving 330 60mW white LEDs. The current of each string is 17.8 mA.


Figure 1: Schematic diagram of a 20W LED fluorescent lamp constant current source

Figure 2 is an actual photo of the constant current source. 33 components are mounted on a 235×25×0.8 mm single-sided epoxy printed circuit board. The PCB routing is designed according to power electronics specifications and can be directly installed in a 28 mm lamp tube.

Figure 2: Actual photo of 20W LED fluorescent lamp constant current source

Electrical parameters and BOM

The main electrical parameters of this constant current source are shown in Table 1. The parameters in the table are obtained by testing in CCM mode. It is designed for 85~245V AC power supply. In fact, it can work in a wider voltage range, such as 60~270V, but the output current will change. The output voltage of driving LEDs from different manufacturers will change slightly. This is caused by the different forward voltage drops of LEDs and will not affect the constant current accuracy. Changing the oscillation frequency and component parameters will cause the circuit to change its working state. For example, reducing the frequency or reducing the inductance of L3 will cause the circuit to enter DCM mode, and the electrical parameters of the circuit will change. The components of the circuit have made a compromise in terms of cost and reliability, and the number of components has been reduced to a minimum. Table 2 is a detailed material list. In order to ensure quality, try to use components from recommended manufacturers.

Test waveform

Figure 3 is the waveform of the emitter of the electronic filter T1. The output voltage is 16V DC. The input voltage is in the range of 70V to 245V, and this voltage is stable.


Figure 3: Base voltage

Figure 4 is the waveform of the MOS tube gate, which is a typical gate drive pulse waveform. The frequency is basically fixed, and the duty cycle of the pulse changes with the load current and input voltage. When the load is fixed, the duty cycle increases as the input voltage decreases, and the duty cycle at the lowest operating voltage is 0.48. The pulse amplitude is fixed at 14.8V and should not increase with the increase of input voltage. In the measurement, it can be seen that the pulse jitters in the horizontal direction. This is not a fault, but a spread spectrum function has been added to the chip to reduce EMI.

Figure 4: Gate signal waveform

Figure 5 is the drain voltage waveform of the MOS tube. The waveform frequency is the same as the gate, but the polarity is opposite. When the constant current source is unloaded, the drain voltage is 1.4 times the AC input voltage, and when loaded, it is 1.2 to 1.3 times the AC input voltage. Due to the use of ultra-high-speed recovery diodes for freewheeling, the reverse electromotive force generated by the inductor is damped, so the waveform is very clean. Note that when using an oscilloscope to test the drain voltage, a special high-voltage probe must be used, otherwise the oscilloscope will be damaged.


Figure 5: Drain signal waveform


Figure 6 is the source voltage of the MOS tube. This voltage is the voltage drop of the working current of the MOS tube on the sensing resistor. Its amplitude is proportional to the working current of the MOS tube. This voltage is sent to the chip as a control signal in a single cycle to control the duty cycle of the gate pulse of the MOS tube so that the current flowing through the LED is constant. The biggest difference between the source voltage and the gate voltage is that there are spikes on the front and back edges of the pulse. The spikes are generated by the output ballast inductor and the parasitic inductance of the MOS tube. These spikes are the source of switching losses. The slope at the top of the waveform is generated by conduction loss. Conduction loss and switching loss are the main causes of MOS tube heating.


Figure 6: Source sampling signal waveform

Figure 7 The two waveforms on the upper left are the voltage waveforms of LED+ and LED- respectively (with 240 ohm load), and the waveform of (LED+)-(LED-) on the lower left is the output voltage. The right figure is the output current ripple measured by the current induction loop. Since the high-frequency response of the current loop is very good, it shows a peak current of tens of millivolts. They are caused by the reverse electromotive force generated by the parasitic inductance of the loop, and the filter capacitor can do nothing about it. Note that a special current probe or current induction loop must be used to measure the current with an oscilloscope.


Figure 7: Output current waveform

Figure 8 shows the output current corresponding to different input voltages in a 27OC room temperature environment, that is, the input voltage regulation rate characteristics.


Figure 8: Input voltage regulation

Figure 9 shows the effect of ambient temperature change on output current. This curve is fitted using test data in Origin software. The test data comes from 10 circuit boards shown in Figure 2 in an aging box, working under load at -15OC to +75OC, with a step length of 5OC.


Figure 9: Temperature-output current characteristics

Instructions

Note: This constant current source is a non-isolated structure. The circuit board and LED pins are energized. Strictly abide by the live safety operation rules to avoid electric shock accidents!

First, check the series and parallel structure of the LED on the LED board. Each string of LEDs must be within the range of 12 to 28, 10 to 15 series and parallel, the total current is controlled within 260mA, and the total power should not exceed 20W. The constant current source board uses a 2-wire power cord to connect to the 220V mains, L to the live wire, and N to the ground wire. The mains is allowed to fluctuate by ±15%. After connecting the LED, turn on the power. It is not recommended to power on first and then connect the LED, as this will damage the LED and shorten its service life. When the LED is lit, if the current deviates from the design value, connect an ammeter with a range greater than 2A in series in the output circuit, and adjust the potentiometer on the circuit board to fine-tune the output current. After the current is adjusted, drip silicone on the potentiometer screw to fix it to prevent vibration from affecting the potentiometer. If the required current value cannot be obtained by adjusting the potentiometer, resistors R6 to R9 can also be changed. Since the heat dissipation setting is designed based on a maximum output power of 20W, do not increase the output power at will. The circuit board can be used directly in production. The Gerber file of the PCB board can be downloaded directly from the PowThch website or requested from the Application System Department, saving design time and cost.

Precautions

Electronic voltage regulator

The circuit that powers U1 is called a capacitor-multiplied ripple filter, which is an effective power purifier. It has the dual functions of a capacitor-multiplied low-pass filter and a series voltage regulator, also called an ACR (Amplificatory Capacitance Regulator) circuit. A capacitor C4 is connected from the base of the emitter output to the ground. Since the base current is only 1/(1+β) of the emitter current, it is equivalent to connecting a large capacitor (1+β) C4 to the emitter. This is the principle of the capacitor-multiplied filter. If a Zener diode is connected from the base to the ground, it is a simple series voltage regulator. Therefore, this circuit has the dual functions of voltage regulation and filtering, and can effectively eliminate high-frequency switching ripples. Note that the Vbceo of the bipolar transistor should be > 500V, Ic = 100mA. The voltage regulator diode D4 uses any type of low-power voltage regulator of 16~18V, 1/4W.


Figure 10: Double capacitance ripple

Power Factor Correction Circuit

The input voltage of the ordinary AC-DC circuit with direct smoothing and filtering after bridge rectification is a sine wave. Since the capacitor charges quickly and discharges slowly, the current is a discontinuous pulse wave, with large harmonic distortion and low power factor. This circuit uses a low-cost passive power factor compensation circuit, as shown in Figure 11. This circuit is called a balanced half-bridge compensation circuit. C1 and D1 form one arm of the half bridge, C2 and D3 form the other arm of the half bridge, and D2 and R1 form a charging connection path. Compensation is performed using the valley filling principle. The filter capacitors C1 and C2 are connected in series, and the voltage on the capacitor is charged to half of the input voltage (VAC/2). Once the line voltage drops below VAC/2, the diodes D1 and D3 will be forward biased, so that C1 and C2 begin to discharge in parallel. After using this circuit, the power factor of the system is improved from 0.6 to 0.88~0.9, but it is difficult to exceed 0.92 because there is still a dead zone of about 60 degrees between the input voltage and current.

Figure 11: Balanced half-bridge PFC circuit

Sampling resistor

Resistors R6, R7, R8, and R9 are connected in parallel as the adopted resistors, which can reduce the influence of resistor accuracy and temperature on the output current, and can easily change the resistance value of one or several of them to achieve the purpose of modifying the current. It is recommended to use SMD resistors with a thousandth accuracy and a temperature coefficient of 50ppm. If there are higher requirements for current accuracy and temperature change, it is recommended to use constantan or manganese copper four-terminal special current sampling resistors.

Electrolytic capacitors

Because the life of aluminum electrolytic capacitors is closely related to temperature, the electrolyte loss is accelerated when the temperature rises, and the life of the capacitor will be reduced by half for every 6OC increase in temperature. Although the life of LEDs is up to 50,000 hours, the life of electrolytic capacitors is only 4,000 hours. When the temperature inside the lamp is relatively high, the life of electrolytic capacitors is even lower. Therefore, the life of this drive circuit depends on the electrolytic capacitor.

Power Inductors

The power inductor L3 is a more critical component than the MOS tube, requiring high Q value, large saturation current and small resistance. For a nominal 3.9 millihenry inductor, the Q should be greater than 90 in the frequency range of 40KHz to 100KHz, and the saturation current should be greater than 2 times the operating current. Here, 500 mA is selected, the winding resistance should be less than 2 ohms, and the Curie temperature should be greater than 400oC. The consequences of using inferior inductors are catastrophic. Once the inductor is saturated, the MOS tube, LED, and control chip will burn out instantly. It is recommended to use a power inductor made of microcrystalline material, which can ensure that the constant current source works safely and reliably for a long time.

Keywords:PT4107_DB03 Reference address:Characteristics and principle of PT4107_DB03 full voltage 20W fluorescent lamp switch constant current source

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