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LTC1412 датащи(PDF) 10 Page - Linear Technology |
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LTC1412 датащи(HTML) 10 Page - Linear Technology |
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10 / 16 page ![]() 10 LTC1412 APPLICATIONS INFORMATION quencies above the converter’s Nyquist Frequency. The noise floor stays very low at high frequencies; S/(N + D) becomes dominated by distortion at frequencies far beyond Nyquist. Driving the Analog Input The differential analog inputs of the LTC1412 are easy to drive. The inputs may be driven differentially or as a single- ended input (i.e., the AIN– input is grounded). The AIN+ and AIN– inputs are sampled at the same instant. Any unwanted signal that is common mode to both inputs will be reduced by the common mode rejection of the sample-and-hold circuit. The inputs draw only one small current spike while charging the sample-and-hold capacitors at the end of conversion. During conversion, the analog inputs draw only a small leakage current. If the source impedance of the driving circuit is low then the LTC1412 inputs can be driven directly. As source impedance increases so will acquisition time (see Figure 6). For minimum acquisition time, with high source impedance, a buffer amplifier must be used. The only requirement is that the amplifier driving the analog input(s) must settle after the small current spike before the next conversion starts (settling time must be 50ns for full throughput rate). frequency. For example, if an amplifier is used in a gain of 1 and has a unity-gain bandwidth of 50MHz, then the output impedance at 50MHz should be less than 100 Ω. The second requirement is that the closed-loop bandwidth must be greater than 40MHz to ensure adequate small- signal settling for full throughput rate. If slower op amps are used, more settling time can be provided by increasing the time between conversions. The best choice for an op amp to drive the LTC1412 will depend on the application. Generally applications fall into two categories: AC applications where dynamic specifica- tions are most critical and time domain applications where DC accuracy and settling time are most critical. The following list is a summary of the op amps that are suitable for driving the LTC1412. More detailed information is available in the Linear Technology Databooks and on the LinearView TM CD-ROM. LT ®1223: 100MHz Video Current Feedback Amplifier. 6mA supply current. ±5V to ±15V supplies. Low Noise. Good for AC applications. LT1227: 140MHz Video Current Feedback Amplifier. 10mA supply current. ±5V to ±15V supplies. Low Noise. Best for AC applications. LT1229/LT1230: Dual and Quad 100MHz Current Feed- back Amplifiers. ±2V to ±15V supplies. Low Noise. Good AC specifications, 6mA supply current each amplifier. LT1360: 50MHz Voltage Feedback Amplifier. 3.8mA sup- ply current. ±5V to ±15V supplies. Good AC and DC specifications. 70ns settling to 0.5LSB. LT1363: 70MHz, 1000V/ µs Op Amps. 6.3mA supply cur- rent. Good AC and DC specifications. 60ns settling to 0.5LSB. LT1364/LT1365: Dual and Quad 70MHz, 1000V/ µs Op Amps. 6.3mA supply current per amplifier. 60ns settling to 0.5LSB. Input Filtering The noise and the distortion of the input amplifier and other circuitry must be considered since they will add to the LTC1412 noise and distortion. The small-signal band- SOURCE RESISTANCE ( Ω) 10 0.01 0.1 1 10 100 1k 1412 F06 10k 100k Figure 6. Acquisition Time vs Source Resistance Choosing an Input Amplifier Choosing an input amplifier is easy if a few requirements are taken into consideration. First, to limit the magnitude of the voltage spike seen by the amplifier from charging the sampling capacitor, choose an amplifier that has a low output impedance (<100 Ω) at the closed-loop bandwidth LinearView is a trademark of Linear Technology Corporation. |
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