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MAX843C/D 数据表(PDF) 8 Page - Maxim Integrated Products |
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MAX843C/D 数据表(HTML) 8 Page - Maxim Integrated Products |
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8 / 10 page ![]() Low-Noise, Regulated, -2V GaAsFET Bias 8 _______________________________________________________________________________________ _______________Detailed Description The MAX840/MAX843/MAX844 are low-noise, inverting, regulated charge-pump power supplies designed for biasing GaAsFET devices, such as power-amplifier modules in cellular handsets. The applied input voltage (VIN) is first inverted to a neg- ative voltage at NEGOUT by a capacitive charge pump. This voltage is then regulated by an internal low-noise linear regulator, and appears at OUT (Figure 1). The minimum (most negative) output voltage achievable is the inverted positive voltage, plus the 0.6V required by the post-regulator. For the MAX840, the linear regulator reduces ripple noise induced by the charge-pump inverter to 1mVp-p at VOUT. In addition, the linear regu- lator’s excellent AC rejection attenuates noise from the incoming supply. __________Applications Information Setting the Output Voltage For the MAX840, select either a fixed or adjustable output voltage. Connect FB directly to GND for a fixed -2V output (Figure 2a). Select an alternate output volt- age by connecting FB to the midpoint of a resistor voltage divider from OUT to GND (Figure 2b). VIN must be 0.6V above the absolute value of VOUT to allow proper regulation. The output voltage is calculat- ed from the formula below. Choose R2 to be between 100k Ω and 400kΩ. VOUT = (-0.5V)(1 + R2 / R1) For the MAX843/MAX844, set the output voltage by connecting a resistor voltage divider between OUT and a positive control voltage (VCTRL) (Figure 2c). VOUT = -VCTRL (R2 / R1) Shutdown Mode The MAX840/MAX843/MAX844 feature a shutdown mode that reduces the supply current to 1µA max over temperature (300µA max for the MAX844). When the MAX840/MAX843 are in shutdown, the outputs (OUT, NEGOUT) and the charge-pump oscillator are dis- abled. When the MAX844 is in shutdown, only the lin- ear regulator is disabled and the NEGOUT output remains enabled. However, the charge-pump oscilla- tion frequency is reduced to 20kHz, reducing the available power at NEGOUT. The output voltage at NEGOUT can be used to bias an LCD while in shut- down. Capacitors Use capacitors with low effective series resistance (ESR) to maintain a low dropout voltage (VIN - |VOUT|). The overall dropout voltage is a function of the charge pump’s output resistance and the voltage drop across the linear regulator (N-channel pass transistor). At the 100kHz switching frequency, the charge-pump output resistance is a function of C1 and C2’s ESR. Therefore, minimizing the ESR of the charge-pump capacitors minimizes the dropout voltage. The output resistance of the entire circuit is approxi- mately: ROUT = RO + 4 x ESRC1 + ESRC4 + 1 / (fS x C1) + R(linear regulator) where [RO + R(linear regulator)], the effective resistance of the internal switches and the resistance across the linear regulator, is approximately 71 Ω at VIN = 2.5V, 48 Ω at VIN = 5V, and 40Ω at VIN = 10V. C1, C2, and C3 should be 1µF capacitors with less than 0.8 Ω ESR. C4 should be a 10µF capacitor with less than 0.2 Ω ESR. Smaller capacitor values can be used (C1 = C2 = C3 = 0.22µF, C4 = 4.7µF) with a small increase in output noise and ripple (Figure 2d). All capacitors should be either surface-mount chip tanta- lum or ceramic types. External capacitor values can be adjusted to optimize size and cost. Layout and Grounding Good layout is important, primarily for good noise perfor- mance. Take the following steps to ensure good layout: 1) Mount all components as close together as possible. 2) Keep traces short to minimize parasitic inductance and capacitance. This includes connections to FB. 3) Use a ground plane. Noise and Ripple Measurement Accurately measuring the output noise and ripple is a challenge. Slight momentary differences in ground potential between the MAX840/MAX843/MAX844 circuit and the oscilloscope (which results from the charge pump’s switching action) cause ground currents in the probe’s wires, inducing sharp voltage spikes. For best results, measure directly across the output capacitor (C4). Do not use the ground lead of the oscilloscope probe; instead, remove the probe’s tip cover and touch the ground ring on the probe directly to C4’s ground terminal. You can also use a Tektronix chassis-mount test jack (part no. 131-0258) to connect your scope probe directly. This direct connection gives the most accurate noise and ripple measurement. |
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