THS7001 Datasheet, PDF (16/32 Pages) Texas Instruments – 70-MHz PROGRAMMABLE-GAIN AMPLIFIERS

THS7001, THS7002
70-MHz PROGRAMMABLE-GAIN AMPLIFIERS
SLOS214B – OCTOBER 1998 – REVISED AUGUST 1999
APPLICATION INFORMATION
noise calculations and noise figure (continued)
RS
eRs
en
Noiseless
eni
+
_
eno
IN+
eRf
RF
IN–
eRg
RG
Figure 52. Noise Model
+ ^{Ǹǒ Ǔ} ) ^ǒ ) ^Ǔ ) ^{ǒ ǒ} ø ^ǓǓ ) ) ^ǒ ø ^{Ǔ The total equivalent input noise density (eni) is calculated by using the following equation:}
2
2
2
eni
en
IN
RS
IN– RF RG
4 kTRs 4 kT RF RG
(1)
Where:
k = Boltzmann’s constant = 1.380658 × 10^–23
T = temperature in degrees Kelvin (273 +°C)
R_F || R_G = parallel resistance of R_F and R_G
+ + ǒ ) Ǔ ^{To get the equivalent output noise of the amplifier, just multiply the equivalent input noise density (eni) by the}
overall amplifier gain (A_V).
eno eni AV
e_ni 1
R_F
R_G
(Noninverting Case)
(2)
As the previous equations show, to keep noise at a minimum, small value resistors should be used. As the
closed-loop gain is increased (by reducing R_F + R_G), the input noise can be reduced considerably because of
the parallel resistance term. This leads to the general conclusion that the most dominant noise sources are the
source resistor (R_S) and the internal amplifier noise voltage (e_n). Because noise is summed in a
root-mean-squares method, noise sources smaller than 25% of the largest noise source can be effectively
ignored. This can greatly simplify the formula and make noise calculations much easier to calculate.
By using the low noise preamplifiers as the first element in the signal chain, the input signal’s signal-to-noise
ratio (SNR) is maintained throughout the entire system. This is because the dominant system noise is due to
the first amplifier. This can be seen with the following example:
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