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TPS51117RGYRG4 Datasheet(PDF) 7 Page - Texas Instruments |
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TPS51117RGYRG4 Datasheet(HTML) 7 Page - Texas Instruments |
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7 / 31 page ![]() V OUT + 1 ) R 1 R 2 0.75 V I OUT(LL) + 1 2 L ƒsw V IN * V OUT V OUT V IN TPS51117 www.ti.com...................................................................................................................................... SLVS631B – DECEMBER 2005 – REVISED SEPTEMBER 2009 DETAILED DESCRIPTION (continued) At the beginning of each cycle, the synchronous high-side MOSFET is turned on, or becomes ON state. This MOSFET is turned off, or becomes OFF state, after the internal one shot timer expires. This one shot is determined by VIN and VOUT to keep the frequency fairly constant over the input voltage range at steady state, hence it is called adaptive on-time control or fixed frequency emulated on-time control (see PWM frequency and Adaptive On-Time Control). The MOSFET is turned on again when both feedback information, monitored at VFB voltage, indicates insufficient output voltage AND inductor current information indicates below the overcurrent limit. Repeating the operation in this manner, the controller regulates the output voltage. The synchronous low-side or rectifying MOSFET is turned on each OFF state to keep the conduction loss to a minimum. The TPS51117 supports selectable PWM-only and auto-skip operation modes. If EN_PSV is grounded, the switching regulator is disabled. If the EN_PSV pin is connected to 3.3 V or 5 V, the regulator is enabled with auto-skip mode selected. The rectifying MOSFET is turned off when inductor current information detects zero level. This enables a seamless transition to reduced frequency operation during a light load condition so that high efficiency is maintained over a broad range of load currents. If the EN_PSV pin is floated, it is internally pulled up to 1.95 V, and the regulator is enabled with PWM-only mode selected. The rectifying MOSFET is not turned off when inductor current reaches zero. The converter runs forced continuous conduction mode for the entire load range. System designers may want to use this mode to avoid a certain frequency during a light load condition but with the cost of low efficiency. However, be aware the output has the capability to both source and sink current in this mode. If the output terminal is connected to a voltage source higher than the regulator’s target, the converter sinks current from the output and boosts the charge into the input capacitor. This may cause unexpected high voltage at VIN and may damage the power FETs. DC output voltage can be set by the external resistor divider as follows (refer to Figure 23, Figure 24, and Figure 25). (1) LIGHT LOAD CONDITION WITH AUTO-SKIP FUNCTION If auto-skip mode is selected, the TPS51117 automatically reduces the switching frequency during a light load condition to maintain high efficiency. This reduction of frequency is achieved smoothly and without an increase of Vout ripple or load regulation. Detailed operation is described as follows. As the output current decreases from a heavy load condition, the inductor current is also reduced and eventually comes to the point that its valley touches zero current, which is the boundary between continuous conduction and discontinuous conduction modes. The rectifying MOSFET is turned off when this zero inductor current is detected. Since the output voltage is still higher than the reference at this moment, both high-side and low-side MOSFETs are turned off and wait for the next cycle. As the load current decreases further, the converter runs in discontinuous conduction mode, taking longer time to discharge the output capacitor below the reference voltage. Note the ON time is kept the same as during the heavy load condition. In reverse, when the output current increases from a light load to a heavy load, the switching frequency increases to the preset value as the inductor current reaches to the continuous conduction. The transition load point to light load operation, IOUT(LL) (i.e., the threshold between continuous and discontinuous conduction mode), can be calculated as follows: (2) where f sw is the PWM switching frequency. Switching frequency versus output current in the light load condition is a function of L, f sw, VIN and VOUT, but it decreases almost proportional to the output current from the IOUT(LL) given above. For example, it is about 60 kHz at IOUT(LL)/5 if the PWM switching frequency is 300 kHz. Copyright © 2005–2009, Texas Instruments Incorporated Submit Documentation Feedback 7 Product Folder Link(s) :TPS51117 |
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