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전자부품 반도체 검색엔진( 무료 PDF 다운로드 ) - 데이터시트뱅크

RHF310AK01V 데이터 시트보기 (PDF) - STMicroelectronics

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RHF310AK01V Datasheet PDF : 25 Pages
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RHF310A
Intermodulation distortion product
6.2.1
6.2.2
6.2.3
6.3
4kT RF
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:
4kT R
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
eN o = V12 + V22+ V32+ V4+2 V52 + V62
Equation 2
eN o2 = eN2 × g2 + iN n2 × R22 + iNp2 × R32 × g2 + RR----21--2 × 4kTR 1 + 4kTR 2 + 1 RR----21---2 × 4+kTR 3
The input noise of the instrumentation must be extracted from the measured noise value. The real output noise
value of the driver is shown in Equation 3.
Equation 3
eNo = (Mea sure d)2 (ins trumen tatio n)2
The input noise is called equivalent input noise because 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 fifth terms of Equation 2, you obtain Equation 4.
Equation 4
eNo2 = eN2 × g2 + iN n2 × R22 + iN p2 × R32 × g2 + g × 4kTR2 + 1 RR----21---2 × 4+kTR 3
Measurement of the input voltage noise eN
Assuming a short-circuit on the non-inverting input (R3 = 0), from Equation 4 you can derive Equation 5.
Equation 5
eN o = eN2 × g2 + iN n2 × R22 + g × 4kTR2
To easily extract the value of eN, the resistance R2 must be as low as possible. On the other hand, the gain must
be high enough. R3 = 0 and gain (g) = 100.
Measurement of the negative input current noise iNn
To measure the negative input current noise iNn, R3 is set to zero and Equation 5 is used. This time, the gain
must be lower in order to decrease the thermal noise contribution. R3 = 0 and gain (g) = 10.
Measurement of the positive input current noise iNp
To extract iNp from Equation 3, a resistance R3 is connected to the non-inverting input. The value of R3 must be
selected so that its thermal noise contribution is as low as possible against the iNp contribution. R3 = 100 Ω and
gain (g) = 10.
Intermodulation distortion product
The non-ideal output of the amplifier can be described by the following series of equations.
Vout = C0 + C1Vin + C2V2in + ... + CnVnin
DS6201 - Rev 7
page 13/25

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