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LT1611CS5 数据表(PDF) 5 Page - Linear Technology |
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LT1611CS5 数据表(HTML) 5 Page - Linear Technology |
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5 / 12 page ![]() 5 LT1611 OPERATIO boost converter, generating a negative output voltage, which is directly regulated. The circuit schematic is de- tailed in Figure 3. Only one inductor is required, and the two diodes can be in a single SOT-23 package. Output noise is the same as in a boost converter, because current is delivered to the output only during the time when the LT1611’s internal switch is off. If D2 is replaced by an inductor, as shown in Figure 4, a higher performance solution results. This converter topol- ogy was developed by Professor S. Cuk of the California Institute of Technology in the 1970s. A low ripple voltage results with this topology due to inductor L2 in series with the output. Abrupt changes in output capacitor current are eliminated because the output inductor delivers current to the output during both the off-time and the on-time of the LT1611 switch. With proper layout and high quality output capacitors, output ripple can be as low as 1mVP–P. The operation of Cuk’s topology is shown in Figures 5 and 6. During the first switching phase, the LT1611’s switch, represented by Q1, is on. There are two current loops in operation. The first loop begins at input capacitor C1, flows through L1, Q1 and back to C1. The second loop flows from output capacitor C3, through L2, C2, Q1 and back to C3. The output current from RLOAD is supplied by L2 and C3. The voltage at node SW is VCESAT and at node SWX the voltage is –(VIN + |VOUT|). Q1 must conduct both L1 and L2 current. C2 functions as a voltage level shifter, with an approximately constant voltage of (VIN + |VOUT|) across it. When Q1 turns off during the second phase of switching, the SW node voltage abruptly increases to (VIN + |VOUT|). The SWX node voltage increases to VD (about 350mV). Now current in the first loop, begining at C1, flows through L1, C2, D1 and back to C1. Current in the second loop flows from C3 through L2, D1 and back to C3. Load current continues to be supplied by L2 and C3. An important layout issue arises due to the chopped nature of the currents flowing in Q1 and D1. If they are both tied directly to the ground plane before being combined, switching noise will be introduced into the ground plane. It is almost impossible to get rid of this noise, once present in the ground plane. The solution is to tie D1’s cathode to the ground pin of the LT1611 before the combined cur- rents are dumped into the ground plane as drawn in Figures 4, 5 and 6. This single layout technique can virtually eliminate high frequency “spike” noise so often present on switching regulator outputs. Output ripple voltage appears as a triangular waveform riding on VOUT. Ripple magnitude equals the ripple current of L2 multiplied by the equivalent series resistance (ESR) of output capacitor C3. Increasing the inductance of L1 and L2 lowers the ripple current, which leads to lower output voltage ripple. Decreasing the ESR of C3, by using ceramic or other low ESR type capacitors, lowers output ripple voltage. Output ripple voltage can be reduced to arbitrarily low levels by using large value inductors and low ESR, high value capacitors. VIN VIN –VOUT 1611 F03 SW L1 D1 D2 GND LT1611 C1 C3 C2 1 µF R2 10k R1 NFB SHDN SHUTDOWN + VIN VIN –VOUT 1611 F04 SW L1 L2 D1 GND LT1611 C1 C3 C2 1 µF R2 10k R1 NFB + Figure 3. Direct Regulation of Negative Output Using Boost Converter with Charge Pump Figure 4. L2 Replaces D2 to Make Low Output Ripple Inverting Topology. Coupled or Uncoupled Inductors Can Be Used. Follow Phasing If Coupled for Best Results |
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