| 전자부품 데이터시트 검색엔진 |
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CLC408 데이터시트(PDF) 4 Page - National Semiconductor (TI) |
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CLC408 데이터시트(HTML) 4 Page - National Semiconductor (TI) |
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4 / 12 page ![]() http://www.national.com 4 Typical Performance Characteristics (A v = +2, Rf = 1kΩ, RL = 100Ω, VCC = +5V, T = 25°C, CLC408AJ; unless specified) Long Term Settling Time Time (s) 0.4 -0.4 1 µ 1m 1 0 10 µ 100 µ 10m 100m -0.2 0.2 Closed Loop Output Resistance Frequency (Hz) 100 0.1 10M 100M 10 1 Gain Flatness & Linear Phase Deviation Frequency (Hz) 1M 10M Gain Phase Small Signal Pulse Response Time (10ns/div) 0.20 0.10 -0.20 0 -0.10 Av+2 Av-2 Large Signal Pulse Response Time (10ns/div) 4.0 2.0 -4.0 0 -2.0 Av+2 Av-2 Short Term Settling Time Time (s) 0.2 0.1 -0.2 0 20n 100n 0 -0.1 Vout = 2Vstep 40n 60n 80n IBI, IBN, VOS vs. Temperature Temperature ( °C) 7.0 6.0 1.0 -50 0 100 5.0 4.0 3.0 2.0 VOS 3.5 3.0 1.5 1.0 0.5 2.5 2.0 50 IBI IBN Settling Time vs. Capacitive Load CL (F) 70 60 30 20 10 100p 20p 1000p 50 40 60 50 20 10 0 40 30 Rs 0.05% 0.1% CLC408 OPERATION The CLC408 has a current-feedback (CFB) architecture built in an advanced complementary bipolar process. The key features of current-feedback are: s AC bandwidth is independent of voltage gain s Inherently unity-gain stability s Frequency response may be adjusted with feedback resistor (Rf in Figures 1-3) s High slew rate s Low variation in performance for a wide range of gains, signal levels and loads s Fast settling Current-feedback operation can be explained with a simple model. The voltage gain for the circuits in Figures 1 and 2 is approximately: where: s Av is the DC voltage gain s Rf is the feedback resistor s Z(j ω) is the CLC408’s open-loop transimpedance gain s is the loop gain The denominator of the equation above is approximately 1 at low frequencies. Near the -3dB corner frequency, the interaction between Rf and Z(jω) dominates the circuit performance. Increasing Rf does the following: s Decreases loop gain s Decreases bandwidth s Reduces gain peaking s Lowers pulse response overshoot s Affects frequency response phase linearity V V A 1 R Zj o in v f = + ()ω Zj Rf ω () |
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