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MIC2133 датащи(PDF) 25 Page - Microchip Technology |
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MIC2133 датащи(HTML) 25 Page - Microchip Technology |
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25 / 50 page ![]() 2022 Microchip Technology Inc. and its subsidiaries DS20006653B-page 25 MIC2133 In each switching cycle of both phases of the MIC2133 converter, the inductor valley current is sensed by mon- itoring the VDS voltage across the low-side MOSFET during the off period. There is a 150 ns (typical) blanking period before each current sense signal considered for protection. The blanking period improves noise immu- nity. If the valley low-side MOSFET current is greater than the current limit threshold current for seven consec- utive cycles in either phase, then the MIC2133 turns off the high-side MOSFET of both phases and a soft start sequence is triggered after the hiccup timer has expired. This mode of operation, called Hiccup mode, and its pur- pose is to protect the downstream load in case of a hard short. The figure below illustrates the MIC2133 opera- tion during overload conditions. When the load current is increased gradually, the inductor current also increases, as shown in the figure below. When the load current is around the current limit threshold, the high-side and the low-side MOSFET current can be higher than the cur- rent limit, as highlighted in the figure below as Case#1. In Case#1, even though the low-side MOSFET instanta- neous current exceeds the current limit threshold for some duration, the low-side MOSFET current is lower than the current limit at the end of the blanking time of 150 ns. This causes the MIC2133 to not enter the cur- rent limit protection and initiate the next high-side MOS- FET turn-on cycle. After the high-side MOSFET is turned on, the current ramps up to a value that is determined by the operating duty cycle and inductor value. When the high-side MOSFET is turned off and the low-side MOS- FET is turned on, as shown as Case#2 in the figure below, the current through the low-side MOSFET is higher than the current limit for seven consecutive cycles. This causes the MIC2133 to enter the current limit protection. As shown in the figure below, the inductor valley current is higher than the current limit threshold as the MIC2133 senses the low-side MOSFET current. When the MIC2133 enters current limit protection, both the high-side and the low-side MOSFETs are turned off for both phases for a hiccup time-out of 2 ms. The inductor current flows through the body diode of the low-side MOSFET until it falls down to zero. The MIC2133 initiates the soft start after the hiccup time-out, as shown in the figure below. FIGURE 4-11: MIC2133 Current-Limit Threshold Relationship to Output Current. The MIC2133 current limit needs to be temperature- insensitive when precise sense resistors or RDSON of the low-side MOSFETs are used. The RDSON resistance increases to about two times from 25°C to 125°C; therefore, an external NTC resis- tor is used to program the current limit in this case. In case regular precise sense resistors are used, no NTC resistance is needed. To achieve a positive temperature coefficient from the negative temperature coefficient of the NTC resistance, the current limit per phase was internally generated, as shown in the equation below. EQUATION 4-16: From Equation 4-16, one can derive the VILIM value through the equation below: EQUATION 4-17: To program the target VILIM voltage, the equation below is used. EQUATION 4-18: EXAMPLE 4-2: CALCULATION OF RILIM FOR BOTTOM MOSFET RDSON CURRENT SENSING Blanking time ( 150ns) Current Limit Threshold SW Soft Start sequence starts here Hiccup Timeout ( 2ms) Output Voltage Low side MOSFET current High side MOSFET current ON state OFF state 1 2 3 4 5 7 Short on Output 7 consecutive current limit events Case#1 Case#2 • For ILIM = 10A per phase, RDSON = 10 mΩ at 25°C; using Equation 4-17, VILIM = 1.2V – 4 * 10 mΩ * 10A = 1.2V – 0.4V = 0.8V at 25°C. • To get 0.8V on the ILIM pin with a 9.6 µA constant-current source, we need a programming equivalent resistance of RILIM = 0.8V/9.6 µA = 83.3 kΩ at 25°C. • If the temperature is increased to 125°C, then RDSON at 125°C = 20 mΩ at the same 10A limit. • Therefore, VILIM = 1.2V – 4 * 20 mΩ * 10A = 1.2V – 0.8V = 0.4V at 125°C. Then, RILIM = 0.4V/9.6 µA = 41.7 kΩ at 125°C. ILIM 0.3 0.25 VILIM – RDSON -------------------------------------------- = Where: ILIM = Desired Current Limit per Phase VILIM = Programmable Voltage at ILIM Pin VILIM 1.2V 4 – R DSON ILIM = VILIM ICL RILIM = Where: ICL = 9.6 µA (typical) Constant-Current Source at ILIM Pin RILIM = Current Limit Threshold Voltage Programming Resistance |
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