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AD8337BCPZ-R2 数据表(PDF) 20 Page - Analog Devices |
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AD8337BCPZ-R2 数据表(HTML) 20 Page - Analog Devices |
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20 / 28 page ![]() AD8337 Data Sheet Rev. D | Page 20 of 28 APPLICATIONS INFORMATION PREAMPLIFIER CONNECTIONS Noninverting Gain Configuration The AD8337 preamplifier is an uncommitted current feedback op amp that is stable for values of RFB2 ≥ 100 Ω. See Figure 66 for the noninverting feedback connections. RG PRAO PREAMPLIFIER + – INPP INPN 5 3 4 RFB2 RFB1 Figure 66. AD8337 Preamplifier Configured for Noninverting Gain Two surface-mount resistors establish the preamplifier gain. Equal values of 100 Ω configure the preamplifier for a 6 dB gain and the device for a default gain range of 0 dB to 24 dB. For preamplifier gains ≥2, select a value of RFB2 ≥ 100 Ω and RFB1 ≤ 100 Ω. Higher values of RFB2 reduce the bandwidth and increase the offset voltage, but smaller values compromise stability. If RFB1 ≤ 100 Ω, the gain increases and the input referred noise decreases. Inverting Gain Configuration For applications requiring polarity inversion of negative pulses, or for waveforms that require current sinking, the preamplifier can be configured as an inverting gain amplifier. When configured with bipolar supplies, the preamplifier amplifies positive or negative input voltages with no level shifting of the common- mode input voltage required. Figure 67 shows the AD8337 configured for inverting gain operation. Because the AD8337 is a very high frequency device, stability issues can occur unless the circuit board on which it is used is carefully laid out. The stability of the preamp is affected by parasitic capacitance around the INPN pin. To minimize stray capacitance position the preamp gain resistors, RFB1 and RFB2, as close as possible to the INPN pin. PRAO PREAMPLIFIER + – INPP INPN 5 3 4 RFB2 RFB1 Figure 67. The AD8337 Preamplifier Configured for Inverting Gain DRIVING CAPACITIVE LOADS Because of the large bandwidth of the AD8337, stray capacitance at the output pin can induce peaking in the frequency response as the gain of the amplifier begins to roll off. Figure 68 shows peaking with two values of load capacitance using ±2.5 V supplies and VGAIN = 0 V. –5 0 10 20 15 25 100k 5 FREQUENCY (Hz) 1M 500M 100M 10M CL = 0pF CL = 10pF CL = 22pF VGAIN = 0V NO SNUBBING RESISTOR Figure 68. Peaking in the Frequency Response for Two Values of Output Capacitance with ±2.5 V Supplies and No Snubbing Resistor –5 0 10 20 15 25 100k 5 FREQUENCY (Hz) 1M 500M 100M 10M CL = 0pF CL = 10pF CL = 22pF VGAIN = 0V WITH 20Ω SNUBBING RESISTOR Figure 69. Frequency Response for Two Values of Output Capacitance with a 20 Ω Snubbing Resistor In the time domain, stray capacitance at the output pin can induce overshoot on the edges of transient signals, as shown in Figure 70 and Figure 72. The amplitude of the overshoot is also a function of the slewing of the transient (not shown in Figure 70 and Figure 72). The transition time of the input pulses used for Figure 70 and Figure 72 is deliberately set high at 300 ps to demon- strate the fast response time of the amplifier. Signals with longer transition times generate less overshoot. |
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