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LT1357CS8 数据表(PDF) 9 Page - Linear Technology |
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LT1357CS8 数据表(HTML) 9 Page - Linear Technology |
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9 / 12 page ![]() 9 LT1357 TYPICAL PERFORMANCE CHARACTERISTICS Large-Signal Transient (AV = 1, CL = 10,000pF) Large-Signal Transient (AV = –1) 1357 TA34 1357 TA35 1357 TA36 Large-Signal Transient (AV = 1) APPLICATIONS INFORMATION The LT1357 may be inserted directly into many high speed amplifier applications improving both DC and AC performance, provided that the nulling circuitry is removed. The suggested nulling circuit for the LT1357 is shown below. Offset Nulling 1357 AI01 6 7 V+ V– 4 8 1 2 10k 3 – + LT1357 Layout and Passive Components The LT1357 amplifier is easy to apply and tolerant of less than ideal layouts. For maximum performance (for example, fast settling time) use a ground plane, short lead lengths and RF-quality bypass capacitors (0.01 µFto0.1µF). For high drive current applications use low ESR bypass capacitors (1 µF to 10µF tantalum). Sockets should be avoided when maximum frequency performance is required, although low profile sockets can provide reasonable performance up to 50MHz. For more details see Design Note 50. The parallel combination of the feedback resistor and gain setting resistor on the inverting input can combine with the input capacitance to form a pole which can cause peaking or oscillations. For feedback resistors greater than 5k Ω, a parallel capacitor of value CF > (RG • CIN)/RF should be used to cancel the input pole and optimize dynamic performance. For unity-gain applications where a large feedback resistor is used, CF should be greater than or equal to CIN. Capacitive Loading The LT1357 is stable with any capacitive load. This is accomplished by sensing the load induced output pole and adding compensation at the amplifier gain node. As the capacitive load increases, both the bandwidth and phase margin decrease so there will be peaking in the frequency domain and in the transient response as shown in the typical performance curves.The photo of the small-signal response with 1000pF load shows 50% peaking. The large-signal response with a 10,000pF load shows the output slew rate being limited to 5V/ µs by the short-circuit current. Coaxial cable can be driven directly, but for best pulse fidelity a resistor of value equal to the characteristic impedance of the cable (i.e., 75 Ω) should be placed in |
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