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ADA4530-1ARZ-R7 数据表(PDF) 41 Page - Analog Devices |
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ADA4530-1ARZ-R7 数据表(HTML) 41 Page - Analog Devices |
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41 / 52 page ![]() Data Sheet ADA4530-1 CURRENT NOISE CONSIDERATIONS analog.com Rev. C | 41 of 52 Figure 118. Current Noise Spectral Density The current noise of the ADA4530-1 originates from the saturation current of the ESD diodes. The diode saturation current has an exponential dependence on temperature; therefore, it is expected that the current noise tracks this temperature behavior. The current noise of the ADA4530-1 is characterized over temperature using the transimpedance measurement circuit with a 1 TΩ resistor. The measurements are limited to 85°C because of the maximum operat- ing temperature of the resistor. Figure 119 shows the current noise density at a frequency of 0.1 Hz for all of the test temperatures. It can be useful to calculate an equivalent noise resistance from the current noise density data in Figure 119. This conversion facilitates comparisons between the current noise generated by the ADA4530-1 and the thermal noise of the feedback resistor used in the circuit. Figure 119. Current Noise Density vs. Temperature Figure 120 shows the equivalent noise resistance vs. temperature. From Figure 120, it is easy to determine that the ADA4530-1 con- tributes less noise than a 1 TΩ resistor for temperatures less than 40°C. If the application requires an 85°C operation, the ADA4530-1 contributes as much noise as a 30 GΩ resistor. This example illus- trates the considerable impact of the temperature in determining the noise performance of an application. Figure 120. Equivalent Noise Resistance vs. Temperature In summary, the excellent noise performance of the ADA4530-1 makes it ideal for electrometer applications. For impedances less than 1 TΩ, the amplifier noise is negligible. Also, unlike other amplifiers, the current noise is fully characterized and is free of excessive blowback noise. |
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