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LTC3240 Datasheet(PDF) 9 Page - Linear Technology |
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LTC3240 Datasheet(HTML) 9 Page - Linear Technology |
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9 / 12 page ![]() LTC3240-3.3/LTC3240-2.5 9 3240fb In charge pump mode the value of COUTdirectlycontrolsthe 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. The peak-to-peak output ripple is approximately given by the expression: V I fC RIPPLE P P OUT OSC OUT () • − ≅ 2 where fOSC is the oscillator frequency (typically 1.2MHz) and COUT is the value of the output capacitor. Also, the value and style of the output capacitor can sig- nificantly affect the stability of the LTC3240. As shown in the Block Diagram, the LTC3240 uses a linear 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 storage capacitor. This output capacitor also serves to form the dominant pole of the control loop. To prevent ringing or instability on the LTC3240, it is important to maintain at least 2µF of capacitance over all conditions. Excessive ESR on the output capacitor can degrade the loop stability of the LTC3240. The closed-loop output resistance of the LTC3240 is designed to be 0.5 Ω. For a 100mA load current change, the output voltage will change by about 50mV. If the output capacitor has 0.5 Ω or more of ESR, the closed-loop frequency response will cease to roll off in a simple one-pole fashion and poor load transient response or instability could result. Ceramic capacitors typically have exceptional ESR performance and combined with a tight board layout should yield very good stability and load transient performance. Just 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) in charge pump mode. The input current to the LTC3240 is relatively constant during the input charging phase and the output charging phase but drops to zero during the nonoverlap times. Since the nonoverlap time is small (~25ns), these missing notches result in a small perturbation on the input power supply line. A higher ESR capacitor such as tantalum will have higher input noise than a low ESR ceramic capacitor. Therefore, ceramic capacitors are again recommended for their exceptional ESR performance. Further input noise reduction can be achieved by power- ing the LTC3240 through a very small series inductor as shown in Figure 3. A 10nH inductor will reject the fast current notches, thereby presenting a nearly constant current load to the input power supply. For economy, the 10nH inductor can be fabricated on the PC board with about 1cm (0.4") of PC board trace. Flying Capacitor Selection Warning: A polarized capacitor such as tantalum or alumi- num should never be used for the flying capacitor since its voltage can reverse upon start-up of the LTC3240. Low ESR ceramic capacitors should always be used for the flying capacitor. The flying capacitor controls the strength of the charge pump. A 1µF or greater ceramic capacitor is suggested for the flying capacitor. For the LTC3240-3.3 operating at an input voltage in the range 1.8V ≤ VIN ≤ 2.5V, it is necessary to have at least 0.5µF of capacitance for the flying capacitor in order to achieve the maximum rated current of 40mA. For very light load applications, the flying capacitor may be reduced to save space or cost. From the first order approximation of ROL in the “Effective Open-Loop Output Resistance” section, the theoretical minimum output resistance of a voltage doubling charge pump can be expressed by the following equation: R VV If C OL MIN IN OUT OUT OSC FLY () – • =≅ 21 where fOSC is the switching frequency (1.2MHz) and CFLY is the value of the flying capacitor. The charge pump will typically be weaker than the theoretical limit due Figure 3. 10nH Inductor Used for Additional Input Noise Reduction APPLICATIO S I FOR ATIO LTC3240-3.3/ LTC3240-2.5 0.22 µF 2.2 µF VIN GND 1cm OF WIRE 10nH VIN 1 2 3240 F03 |
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