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RHF330 датащи(PDF) 14 Page - STMicroelectronics |
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RHF330 датащи(HTML) 14 Page - STMicroelectronics |
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14 / 22 page ![]() Noise measurements RHF330 14/22 Doc ID 15576 Rev 3 5 Noise measurements The noise model is shown in Figure 30. ● eN: input voltage noise of the amplifier ● iNn: negative input current noise of the amplifier ● iNp: positive input current noise of the amplifier Figure 30. Noise model The thermal noise of a resistance R is: where ΔF is the specified bandwidth. On a 1 Hz bandwidth the thermal noise is reduced to: where k is the Boltzmann's constant, equal to 1,374.E(-23)J/°K. T is the temperature (°K). 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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