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LTC3203 Datasheet(PDF) 12 Page - Linear Technology |
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LTC3203 Datasheet(HTML) 12 Page - Linear Technology |
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12 / 16 page ![]() LTC3203/LTC3203-1 LTC3203B/LTC3203B-1 12 32031fa APPLICATIO S I FOR ATIO For the example given, a 5V output setting with ±4% output tolerance and maximum load current of 500mA, a resistor ratio of: R R MODE MODE 1 2 4 > at the MODE pin allows the chip to switch modes while maintaining regulation. VIN, VOUT Capacitor Selection The style and value of capacitors used with the LTC3203/LTC3203-1/LTC3203B/LTC3203B-1 determine several important parameters such as regulator control loop stability, output ripple, charge pump strength and minimum start-up time. To reduce noise and ripple, it is recommended that low equivalent series resistance (ESR) multilayer ceramic chip capacitors (MLCCs) be used for both CIN and COUT. Tanta- lum and aluminum capacitors are not recommended be- cause of their high ESR. In 1.5x mode, the value of COUT directly controls the amount of output ripple for a given load current. Increasing the size of COUT will reduce the output ripple at the expense of higher minimum turn-on time and higher start-up cur- rent. The peak-to-peak output ripple for 1.5x mode is given by the expression: V I fC RIPPLE P P OUT OSC OUT () − = • 3 where fOSC is the LTC3203/LTC3203-1/LTC3203B/ LTC3203B-1’s oscillator frequency (typically 0.9MHz) and COUT is the output charge storage capacitor. In 2x mode, the output ripple is very low due to the out-of- phase operation of the two flying capacitors. VOUT remains almost flat when either of the flying capacitors is connected to VOUT. Both the type and value of the output capacitor can signifi- cantly affect the stability of the LTC3203/LTC3203-1/ LTC3203B/LTC3203B-1. As shown in the Block Diagram, the LTC3203/LTC3203-1/LTC3203B/LTC3203B-1 use a control loop to adjust the strength of the charge pump to match the current required at the output. The error signal of this loop is stored directly on the output charge storage capacitor. The charge storage capacitor also serves to form the dominant pole for the control loop. To prevent ringing or instability, it is important for the output capaci- tor to maintain at least 4.7 µF of capacitance over all conditions. Note that the actual capacitance of ceramic capacitors usually drops when biased with DC voltage. Different capacitor types drop to different extents. Make sure that the selected ceramic capacitors have enough capacitance when biased with the required DC voltage. Likewise, excessive ESR on the output capacitor will tend to degrade the loop stability of the LTC3203/LTC3203-1/ LTC3203B/LTC3203B-1. The closed-loop output resis- tance of the LTC3203/LTC3203-1/LTC3203B/LTC3203B- 1 are designed to be 0.27 Ω (at 1.5x mode). For a 100mA load current change, the output voltage will change by about 27mV. If the output capacitor has 0.27 Ω or more of ESR, the closed-loop frequency response will cease to roll-off in a simple one-pole fashion and poor load tran- sient response or instability could result. Multilayer ce- ramic chip capacitors typically have exceptional ESR per- formance and, combined with a good board layout, should yield very good stability and load transient performance. As the value of COUT controls the amount of output ripple, the value of CIN controls the amount of ripple present at the input pin (VIN). The input current to the LTC3203/ LTC3203-1/LTC3203B/LTC3203B-1 will be relatively con- stant while the charge pump is on either the input charging phase or the output charging phase but will drop to zero during the clock non-overlap times. Since the non-overlap time is small (~40ns) these missing “notches” will result in only a small perturbation on the input power supply line. Note that a higher ESR capacitor such as tantalum will have higher input noise by the amount of the input current change times the ESR. Therefore ceramic capacitors are again recommended for their exceptional ESR performance. Further input noise reduction can be achieved by powering the LTC3203/LTC3203-1/LTC3203B/ LTC3203B-1 through a very small series inductor as shown in Figure 5. |
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