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AN4461 Datasheet(PDF) 20 Page - STMicroelectronics |
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AN4461 Datasheet(HTML) 20 Page - STMicroelectronics |
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20 / 70 page ![]() ZVS LC resonant stage description AN4461 20/70 DocID026130 Rev 2 Step 3: Calculate the inductance value of the Lres, which is given by Equation 8 and Equation 13: Equation 15 Step 4: determine the capacitance value of the resonant capacitor Cres so that the peak amplitude of the AC ripple voltage is much lower (e.g. always 10%) than the DC offset. Indicatively: Equation 16 Step 5: select the output capacitors Co so that they are rated for the maximum output voltage VLED, they meet the output voltage ripple specification (if any) and have an adequate AC current ripple rating. The output current ripple specification must be met. To do so, at first we need to find the value of the overall RLED for the LED string by considering the tangent to the forward characteristic in the specified operating point. Then Equation 17 can be used to find the suitable value for Co and its ESR. Equation 17 The maximum allowed ripple current for Co must be: Equation 18 4.1.3 Half-bridge operating parameters In order to generate a proper oscillation into the LC resonant tank, the half-bridge must generate a square wave having a 50% of duty cycle. Any unbalancing of this duty cycle may cause the loss of zero voltage switching condition and, as a consequence, increases the risk of components overstress. The adoption of the same conduction time (TON) for both the halfbridge MOSFETs ensures this condition. When one MOSFET is turned off then the middle point of the half-bridge, thanks to resonance, moves to the opposite side of the half-bridge, in a time that depends on the overall capacitance (real or parasitic) connected to this node. In order to avoid undesired switching losses, a deadtime (see “hf” command), longer than this transition time, shall be applied between the time one side of the half-bridge switches off and the time the opposite side turns on. In order to correctly regulate the LED current, it is important to accurately detect the instant of the peak of the resonant current. The peak is detected by the STLUX385A via a shunt resistor placed between the source of the low-side MOSFET and ground. The sampling time ( ) ( ) Vdout VLED min Vpfc, f ILED 32 λ - 1 λ Lres 2 min hb, 2 + ⋅ ⋅ ⋅ = min hb, f min Vpfc, n ILED 5 Cres ⋅ ⋅ ≥ 2 2 min hb, ESR 4 f Co 4 1 RLED ILED ILED ⋅ + ⋅ ⋅ ≥ ⋅ ∆ 3 ILED ∆ICo ≥ |
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