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PFS7523L/H 数据表(PDF) 15 Page - Power Integrations, Inc. |
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PFS7523L/H 数据表(HTML) 15 Page - Power Integrations, Inc. |
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15 / 37 page ![]() Rev. D 04/25 15 PFS7523-7529/7533-7539 www.power.com Design, Assembly, and Layout Considerations Power Table The data sheet power table as shown in Table 2 represents the maximum practical continuous output power based on the following conditions: For the universal input devices (PFS7523L/H – PFS7529H): 1. An input voltage range of 90 VAC to 264 VAC. 2. Overall efficiency of at least 93% at the lowest operating voltage. 3. 385 V nominal output. 4. Sufficient heat sinking to keep device temperature ≤100 ºC. Operation beyond the limits stated above will require derating. Operation at elevated temperatures could result in reduced MTBF and performance degradation, e.g. reduced efficiency, reduced power limit, PF, and potential of observing hysteretic brown-out, etc., and is not recommended. Use of a nominal output voltage higher than 395 V is not recommended for HiperPFS-3 based designs. Operation at voltages higher than 395 V can result in higher than expected drain-source voltage during line and load transients. HiperPFS-3 Selection Selection of the optimum HiperPFS-3 part depends on required maximum output power, PFC efficiency and overall system efficiency (when used with a second stage DC-DC converter), heat sinking constraints, system requirements and cost goals. The HiperPFS-3 part used in a design can be easily replaced with the next higher or lower part in the power table to optimize performance, improve efficiency or for applications where there are thermal design constraints. Minor adjustments to the inductance value and EMI filter components may be necessary in some designs when the next higher or the next lower HiperPFS-3 part is used in an existing design for performance optimization. Every HiperPFS-3 family part has an optimal load level where it offers the most value. Operating frequency of a part will change depending on load level. Change of frequency will result in change in peak to peak current ripple in the inductance used. Change in current ripple will affect input PF and total harmonic distortion of input current. Input Fuse and Protection Circuit The input fuse should be rated for a continuous current above the input current at which the PFC turns-off due to input under- voltage. This voltage is referred to as the brown-out voltage. The fuse should also have sufficient I2t rating in order to avoid nuisance failures during start-up. At start-up a large current is drawn from the input as the output capacitor charges to the peak of the applied voltage. The charging current is only limited by any inrush limiting thermistors, impedance of the EMI filter inductors and the forward resistance of the input rectifier diodes. A MOV will typically be required to protect the PFC from line surges. Selection of the MOV rating will depend on the energy level (EN1000-4-5 Class level) which the PFC is required to withstand. A suitable NTC thermistor should be used on the input side to provide inrush current limiting. Choice of this thermistor should depend on the inrush current specification for the power supply. NTC thermis- tors may not be placed in any other location in the circuit as they fail to limit the stress on the part in the event of line transients and also fail to limit the inrush current in a predictable manner. The example in Figure 13 shows the circuit configuration that has the inrush limiting NTC thermistor on the input side which is bypassed with a relay after PFC start-up. This arrangement ensures that a consistent inrush limiting performance is achieved by the circuit. Input EMI Filter The variable switching frequency of the HiperPFS-3 effectively modulates the switching frequency and reduces conducted EMI peaks associated with the harmonics of the fundamental switching frequency. This is particularly beneficial for the average detection mode used in EMI measurements. The PFC is a switching converter and will need an EMI filter at the input in order to meet the requirements of most safety agency standards for conducted and radiated EMI. Typically a common mode filter with X capacitors connected across the line will provide the required attenuation of high frequency components of input current to an acceptable level. The leakage reactance of the common mode filter inductor and the X capacitors form a low pass filter. In some designs, additional differential filter inductors may have to be used to supplement the differential mode inductance of the common-mode choke. A filter capacitor with low ESR and high ripple current capability should be connected at the output of the input bridge rectifier. This capacitor reduces the generation of the switching frequency compo- nents of the input current ripple and simplifies EMI filter design. Typically, 0.33 µF per 100 W should be used for universal input designs and 0.15 µF per 100 W of output power should be used for 230 VAC only designs. It is often possible to use a higher value of capacitance after the bridge rectifier and reduce the X capacitance in the EMI filter. Regulatory requirements require use of a discharge resistor to be connected across the input X capacitance on the AC side of the bridge rectifier. This is to ensure that residual charge is dissipated after the input voltage is removed when the capacitance is higher than 0.1 µF. Use of CAPZero integrated circuits from Power Integra- tions, helps eliminate the steady- state losses associated with the use of discharge resistors connected permanently across the X capacitors. Inductor Design For ferrite inductors the optimal design has K P of 0.3 to 0.45. (KP is defined as the current peak-to-peak value divided by the peak value at minimum AC voltage and 90* phase angle, full load). K P <0.3 (more continuous) tends towards excessive inductor size, while higher K P >0.45 tends towards excessive winding AC resistance losses due to large high-frequency AC currents, especially since most ferrite inductor designs will require >3 winding layers. Flux density at maximum current limit should be <3900 gauss to prevent core saturation. If Sendust core material is used, 90µ or 125µ material is recommended, because the higher µ materials tend to produce greater inductance at lower currents, and thus reduced peak- to-peak inductor currents at lower line phase angles (<45*) which reduces losses and improves PF at lighter loads and higher input voltages. The design target is for H at the peak current (low-line, full-load, 90* line phase angle) to be ~60 A-t/cm. Higher H tends towards excessive core loss, and lower than this increases AC copper losses. The HiperPFS-3 design spreadsheet simplifies this process and automatically recommends a core size and design for either ferrite or Sendust. For high performance designs, use of Litz wire is recommended to reduce copper loss due to skin effect and proximity effect. For toroidal inductors the numbers of layers should be less than 3 and for bobbin wound inductors, inter layer insulation should be used to minimize inter layer capacitance. |
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