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LTC3872 датащи(PDF) 13 Page - Linear Technology |
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LTC3872 датащи(HTML) 13 Page - Linear Technology |
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13 / 20 page ![]() LTC3872 13 3872fa Power MOSFET Selection. 3. The losses in the inductor are simply the DC input cur- rent squared times the winding resistance. Expressing this loss as a function of the output current yields: P I D R R WINDING OMAX MAX W () () – • = ⎛ ⎝⎜ ⎞ ⎠⎟ 1 2 4. Losses in the boost diode. The power dissipation in the boost diode is: PDIODE = IO(MAX) • VD The boost diode can be a major source of power loss in a boost converter. For the 3.3V input, 5V output at 7A ex- ample given above, a Schottky diode with a 0.4V forward voltage would dissipate 2.8W, which represents 7% of the input power. Diode losses can become significant at low output voltages where the forward voltage is a significant percentage of the output voltage. 5. Other losses, including CIN and CO ESR dissipation and inductor core losses, generally account for less than 2% of the total additional loss. Checking Transient Response The regulator loop response can be verified by looking at the load transient response. Switching regulators generally take several cycles to respond to an instantaneous step in resistive load current. When the load step occurs, VO immediately shifts by an amount equal to ( ΔILOAD)(ESR), and then CO begins to charge or discharge (depending on the direction of the load step) as shown in Figure 6. The regulator feedback loop acts on the resulting error amp output signal to return VO to its steady-state value. During this recovery time, VO can be monitored for overshoot or ringing that would indicate a stability problem. A second, more severe transient can occur when con- necting loads with large (>1μF) supply bypass capacitors. The discharged bypass capacitors are effectively put in parallel with CO, causing a nearly instantaneous drop in VO. No regulator can deliver enough current to prevent this problem if the load switch resistance is low and it is driven quickly. The only solution is to limit the rise time of the switch drive in order to limit the inrush current di/dt to the load. Boost Converter Design Example The design example given here will be for the circuit shown on the front page. The input voltage is 3.3V, and the output is 5V at a maximum load current of 2A. 1. The duty cycle is: D VV V VV OD IN OD = + + ⎛ ⎝⎜ ⎞ ⎠⎟ = + + = –. – . . .% 50 4 3 3 50 4 38 9 2. An inductor ripple current of 40% of the maximum load current is chosen, so the peak input current (which is also the minimum saturation current) is: I I D IN PEAK OMAX MAX () () • – .• – =+ ⎛ ⎝⎜ ⎞ ⎠⎟ = 1 21 12 2 10 χ .. . 39 39 = A The inductor ripple current is: Δ= = = I I D A L OMAX MAX χ • – .• –. . () 1 04 2 10 39 13 And so the inductor value is: L V If D V AkHz IN MIN L MAX = Δ == () • • . .• •. 33 1 3 550 039 1..8 μH The component chosen is a 2.2μH inductor made by Sumida (part number CEP125-H 1ROMH). APPLICATIO S I FOR ATIO Figure 6. Load Transient Response for a 3.3V Input, 5V Output Boost Converter Application, 0.1A to 1A Step IL 500mA/DIV VOUT 200mV/DIV AC COUPLED 20 μs/DIV 3872 F06 |
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