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RHF310 Fiches technique(PDF) 13 Page - STMicroelectronics |
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RHF310 Fiches technique(HTML) 13 Page - STMicroelectronics |
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13 / 22 page ![]() RHF310 Noise measurements Doc ID 15577 Rev 3 13/22 4 Noise measurements The noise model is shown in Figure 24. ● eN: input voltage noise of the amplifier. ● iNn: negative input current noise of the amplifier. ● iNp: positive input current noise of the amplifier. Figure 24. Noise model The thermal noise of a resistance R is: where ΔF is the specified bandwidth, and k is the Boltzmann's constant, equal to 1,374.10-23J/°K. T is the temperature (°K). On a 1 Hz bandwidth the thermal noise is reduced to: The output noise eNo is calculated using the superposition theorem. However, eNo is not the simple sum of all noise sources but rather the square root of the sum of the square of each noise source, as shown in Equation 1. Equation 1 + _ R3 R1 Output R2 iN - iN + HP3577 Input noise: 8 nV/ √Hz N1 N2 N3 eN AM00837 4kTR ΔF 4kTR eNo V1 2 V2 2 V3 2 V4 2 V5 2 V6 2 +++++ = |
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