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L6599ATDTR 数据表(PDF) 19 Page - STMicroelectronics |
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L6599ATDTR 数据表(HTML) 19 Page - STMicroelectronics |
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19 / 31 page ![]() L6599AT Application information Doc ID 15534 Rev 3 19/31 Equation 5 where fstart is recommended to be at least 4 times fmin. The proposed criterion for CSS is quite empirical and is a compromise between an effective soft-start action and an effective OCP (see next section). Please refer to the timing diagram of Figure 10 to see some significant signals during the soft-start phase. 6.4 Current sense, OCP and OLP The resonant half-bridge is essentially voltage-mode controlled; hence a current sense input only serves as overcurrent protection (OCP). Unlike PWM-controlled converters, where energy flow is controlled by the duty cycle of the primary switch (or switches), in a resonant half-bridge the duty cycle is fixed and energy flow is controlled by its switching frequency. This impacts the way current limitation can be realized. While in PWM-controlled converters energy flow can be limited simply by terminating switch conduction beforehand when the sensed current exceeds a preset threshold (this is commonly known as cycle-by-cycle limitation), in a resonant half-bridge the switching frequency (that is, its oscillator frequency) must be increased and this cannot be done as quickly as turning off a switch: it takes at least the next oscillator cycle to see the frequency change. This implies that to have an effective increase, capable of changing the energy flow significantly, the rate of change of the frequency must be slower than the frequency itself. This, in turn, implies that cycle-by-cycle limitation is not feasible and that, therefore, the information on the primary current fed to the current sensing input must be somehow averaged. Of course, the averaging time must not be too long, to prevent the primary current from reaching excessively high values. In Figure 11, a few current sensing methods are illustrated that are described in the following paragraphs. The circuit in Figure 11a is more simple, but the dissipation on the sense resistor Rs may not be negligible, decreasing efficiency. The circuit in Figure 11b is more complex, but virtually lossless and recommended when the efficiency target is very high. SS 3 SS min start min SS R 10 3 C ; 1 f f RF R − ⋅ = − = |
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