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HVLED007 数据表(PDF) 11 Page - STMicroelectronics |
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HVLED007 数据表(HTML) 11 Page - STMicroelectronics |
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11 / 33 page ![]() DS12866 Rev 1 11/33 HVLED007 Application information 33 Note that in Equation 2 also TON is denoted as a function of the instantaneous line phase θ; in fact, with the novel method it is no longer constant as in the traditional method. The "Input Current Shaper" (ICS) that implements this basic idea is shown in Figure 5 along with the overall control loop inside the IC. Figure 5. Input current shaper (ICS) block and its interconnection with HVLED007 control The ON/OFF mechanism of the external power switch is exactly the same as in the traditional TM method: the power switch is turned on as the secondary current zeroes (with a delay TR to achieve valley switching, see "Section 4.8: Zero current detection and triggering block (pin ZCD); starter") and turned off when the voltage Vcs (t, θ) on the current sensing input CS (proportional to the primary current Ip (t, θ)) reaches the reference value Vcsref (θ). Note that the explicit dependence on time (t) denotes cycle-by-cycle quantities. The difference between the traditional TM method and that implemented in the HVLED007 is in the way the reference Vcsref (θ) is generated. In the traditional TM method, Vcsref (θ) is generated by taking the input voltage as the template and adjusting its amplitude with feedback loop control voltage via the multiplier; in the HVLED007 the output of the multiplier is processed by the ICS circuit highlighted in the dotted box before being provided to the PWM comparator. The ICS circuit is composed of the current generator IMULT (θ), the external capacitor Ct connected between pin CT and ground and a switched resistor Rt that is connected in parallel to Ct during the ON-time TON (θ) of the power switch through the switch SW. The current generator provides the charging current for Ct, given by: Equation 3 where Kp = RmultL / (RmultH + RmultL) is the voltage gain of the resistor divider that senses the rectified input voltage. The key waveforms are shown in Figure 6. Assuming T(θ) << Rt Ct << 1/(2 fline), to a first approximation the voltage ripple across the capacitor Ct can be neglected and the current IMULT (θ) can be considered constant in a switching cycle. The average voltage VCt (θ) developed across Ct, which shapes the peak primary current Ippk(θ), is found by charge balance in a switching cycle: S R Q Vcs t Q Rt Ct IMULT kI Vc VMULT Vc Vcsref VZf Vcsmax Rf Cf VMULT SW kI RCOMP VCt FW RmultH RmultL Rs Ip t IMULT = k I K p V inpk sin V c |
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