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LTC3113 数据表(PDF) 12 Page - Linear Technology |
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LTC3113 数据表(HTML) 12 Page - Linear Technology |
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12 / 24 page ![]() LTC3113 12 3113f APPLICATIONS INFORMATION The basic LTC3113 application circuit is shown as the typical application on the front page of this data sheet. The external component selection is dependent upon the required performance of the IC in each particular appli- cation given considerations and trade-offs such as PCB area, output voltage, output current, output ripple voltage and efficiency. This section of the data sheet provides some basic guidelines and considerations to aid in the selection of external components and the design of the application circuit. OUTPUT VOLTAGE PROGRAMMING The buck-boost output voltage is set via an external resistor divider connected to the FB pin as shown in Figure 2. formulas, where f is the frequency in MHz and L is the inductance in μH: ΔI L,P-P,BUCK = V OUT f• L V IN –VOUT V IN ⎛ ⎝⎜ ⎞ ⎠⎟ A () ΔI L,P-P,BOOST = V IN f• L V OUT –VIN V OUT ⎛ ⎝⎜ ⎞ ⎠⎟ A () To ensure operation without triggering the reverse current comparator under no load conditions it is recommended that the peak-to-peak inductor ripple not exceed 800mA taking into account the maximum reverse current limit of –0.4A specified in the Electrical Characteristics section. Utilizing this recommendation for applications operating at a switching frequency of 300kHz requires a minimum inductance of 6.8μH, similarly an application operation at a frequency of 2MHz would require a minimum of 1μH. In addition to affecting output current ripple, the value of the inductor can also impact the stability of the feedback loop. In boost and buck-boost mode, the converter transfer function has a right half plane zero at a frequency that is inversely proportional to the value of the inductor. As a result, a large inductor can move this zero to a frequency that is low enough to degrade the phase margin of the feedback loop. In addition to affecting the efficiency of the buck-boost converter, the inductor DC resistance can also impact the maximum output capability of the buck-boost converter at low input voltage. In buck mode, the buck-boost output current is limited only by the inductor current reaching the current limit value. However, in boost mode, especially at large step-up ratios, the output current capability can also be limited by the total resistive losses in the power stage. These include switch resistances, inductor resistance and PCB trace resistance. Use of an inductor with high DC resistance can degrade the output current capability from that shown in the graph in the Typical Performance Characteristics section of this data sheet. Different inductor core materials and styles have an impact on the size and price of an inductor at any given current rating. Shielded construction is generally preferred as it minimizes the chances of interference with other circuitry. FB R1 3113 F02 R2 LTC3113 1.8V ≤ VOUT ≤ 5.5V SGND Figure 2. Setting the Output Voltage The resistor divider values determine the buck-boost output voltage according to the following formula: V OUT = 0.600 1+ R2 R1 ⎛ ⎝⎜ ⎞ ⎠⎟ V () As noted in the Current Limit Operation section: “for the current limit feature to be most effected, the Thevenin re- sistance (R1||R2) from FB to ground should exceed 100k.” INDUCTOR SELECTION To achieve high efficiency, a low ESR inductor should be selected for the buck-boost converter. In addition, the inductor must have a saturation current rating that is greater than the worst-case average inductor current plus half the ripple current. The peak-to-peak inductor current ripple will be larger in buck and boost mode than in the buck-boost region. The peak-to-peak inductor current ripple for each mode can be calculated from the following |
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