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L6572 Datasheet(PDF) 16 Page - STMicroelectronics |
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L6572 Datasheet(HTML) 16 Page - STMicroelectronics |
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16 / 22 page ![]() Application information L6572 16/22 Doc ID 023882 Rev 1 6 Application information 6.1 Target applications The L6572 is primarily intended to accurately drive, with a minimum number of external components, integrated compact fluorescent lamps. Its particular current control method allows a noticeable extension of lamp lifetime and a higher light quality compared to that obtainable by self oscillating ballasts. Also, the operation of the application during normal operation is very similar to the above mentioned ballasts, but with an improved repeatability of the lamp parameters (see Figure 2). The same advantages can be exploited by separately controlled fluorescent lamp applications, especially CFLs up to 26 W. Using further external components, higher power ratings are also reachable. Furthermore, dimming functionality, in particular two-step dimming, helps to implement variable light sources. 6.2 Designing a simple fixed power CFLi application using the L6572 The first step to follow is to define the clock frequency: it can be calculated in order to fit the preheating time requirements. The following equations give the relationships between the typical value of clock period, the preheating time and RCL value. ● ● ● Given the clock frequency, the value of the resonance frequency of the LC cell must be selected higher than the half of the clock frequency in all possible conditions. Otherwise the ignition recognition circuitry may operate incorrectly. ● The range of frequencies related to nominal operation and to the preheating phase can be now selected respectively below and above FRes. Considering the operating frequency ranges and the lamp parameters, the value for resonant components can now be selected: different calculation approaches can be adopted.The value of the sense resistor has to be chosen in order to guarantee a sufficient signal level for the ZCD function: at minimum the peak of the resonant current in every condition must be above VZVS. As the reference current of programming resistors is matched the integrator reference current, a relation between the programming resistor value and the obtained voltage*time area (VTA) can be expressed. These relations can be used to evaluate a first tentative value for the programming resistors RPH, RNO and RDO. A subsequent iterative verification on the real project is usually required: in fact, the value of the integral is highly dependent on the real shape of the sense voltage. Deadtime duration somewhat affects the result of the integration as well. RCL k Ω 0.10327 T PH ms ⋅ ≅ TCLμs 0.2364 RCLkΩ ⋅ ≅ FCL KHZ 1000 TCLμs ----------------- ≅ F Res 1 2 π LC ⋅ ⋅ --------------------------------- ≅ |
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