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LT1055MH Datasheet(PDF) 10 Page - Linear Technology |
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LT1055MH Datasheet(HTML) 10 Page - Linear Technology |
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10 / 16 page ![]() 10 LT1055/LT1056 10556fc APPLICATIONS INFORMATION The voltage noise spectrum is characterized by a low 1/f corner in the 20Hz to 30Hz range, significantly lower than on other competitive JFET input op amps. Of particular interest is the fact that with any JFET IC amplifier, the frequency location of the 1/f corner is proportional to the square root of the internal gate leakage currents and, therefore, noise doubles every 20 °C. Furthermore, as illustrated in the noise versus chip temperature curves, the 0.1Hz to 10Hz peak-to-peak noise is a strong function of temperature, while wideband noise (f0 = 1kHz) is practically unaffected by temperature. Consequently, for optimum low frequency noise, chip temperature should be minimized. For example, operating an LT1056 at ±5V supplies or with a 20°C/W case-to- ambient heat sink reduces 0.1Hz to 10Hz noise from typically 2.5 µVP-P (±15V, free-air) to 1.5µVP-P. Similiarly, the noise of an LT1055 will be 1.8 µVP-P typically because of its lower power dissipation and chip temperature. High Speed Operation Settling time is measured in the test circuit shown. This test configuration has two features which eliminate prob- lems common to settling time measurments: (1) probe capacitance is isolated from the “false summing” node, and (2) it does not require a “flat top” input pulse since the input pulse is merely used to steer current through the diode bridges. For more details, please see Application Note 10. As with most high speed amplifiers, care should be taken with supply decoupling, lead dress and component placement. When the feedback around the op amp is resistive (RF), a pole will be created with RF, the source resistance and capacitance (RS, CS), and the amplifier input capacitance (CIN ≈ 4pF). In low closed-loop gain configurations and with RS and RF in the kilohm range, this pole can create excess phase shift and even oscillation. A small capacitor (CF) in parallel with RF eliminates this problem. With RS (CS + CIN) = RFCF, the effect of the feedback pole is completely removed. 0.01 DISC + + – + 15V 15V –15V –15V 15k 15k 15k 15k 10k 4.7k 4.7k 10 µF SOLID TANTALUM 10 µF SOLID TANTALUM 10 µF SOLID TANTALUM 10 µF SOLID TANTALUM 10pF (TYPICAL) 10k PULSE GEN INPUT (5V MIN STEP) 2k 2k 0.01 DISC 0.01 DISC 0.01 DISC 50 Ω 2W LT1055 LT1056 AMPLIFIER UNDER TEST AUT OUTPUT HP5082-8210 HEWLETT PACKARD 15V 15V 15V –15V = 1N4148 –15V –15V 1/2 U440 1/2 U440 50 Ω 3 Ω 3 Ω 100 Ω DC ZERO 2N160 2N5160 2N3866 2N3866 LT1055/56 AI04 OUTPUT TO SCOPE Settling Time Test Circuit – + RS RF CF CS CIN OUTPUT LT1055/56 AI03 |
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