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TS616 数据表(PDF) 24 Page - STMicroelectronics |
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TS616 数据表(HTML) 24 Page - STMicroelectronics |
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24 / 37 page ![]() Noise measurements TS616 24/37 The output noise eNo is calculated using the Superposition Theorem. However eNo is not the 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 Equation 2 The input noise of the instrumentation must be extracted from the measured noise value. The real output noise value of the driver is: Equation 3 The input noise is called the Equivalent Input Noise as it is not directly measured but is evaluated from the measurement of the output divided by the closed loop gain (eNo/g). After simplification of the fourth and the fifth term of Equation 2 we obtain: Equation 4 7.1 Measurement of eN If we assume a short-circuit on the non-inverting input (R3=0), Equation 4 becomes: Equation 5 In order to easily extract the value of eN, the resistance R2 will be chosen as low as possible. On the other hand, the gain must be large enough: ● R1=10 Ω, R2=910 Ω, R3=0, Gain=92 ● Equivalent input noise: 2.57 nV/ √Hz ● Input voltage noise: eN=2.5 nV/ √Hz NoV1 2 V2 2 V3 2 V4 2 V5 2 V6 2 +++ ++ = No 2 eN 2 g 2 iNn 2 R2 2 iNp 2 + × + × R3 2 × g 2 × = … R2 R1 -------- ⎝⎠ ⎛⎞ 2 4kTR1 4kTR2 1 R2 R1 -------- + ⎝⎠ ⎛⎞ 2 4kTR3 × ++ × + eNo Measured () 2 instrumentation () 2 – = eN 2 g 2 iNn 2 R2 2 iNp 2 + × + × R3 2 × g 2 ×… g4kTR2 1 R2 R1 -------- + ⎝⎠ ⎛⎞ 2 4kT × + × + = NoeN 2 g 2 iNn 2 R2 2 g4kTR2 × + × + × = |
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