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THS7002EVM Datasheet(PDF) 16 Page - Texas Instruments |
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THS7002EVM Datasheet(HTML) 16 Page - Texas Instruments |
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16 / 32 page ![]() THS7001, THS7002 70-MHz PROGRAMMABLE-GAIN AMPLIFIERS SLOS214B – OCTOBER 1998 – REVISED AUGUST 1999 16 POST OFFICE BOX 655303 • DALLAS, TEXAS 75265 APPLICATION INFORMATION noise calculations and noise figure (continued) _ + RF RS RG eRg eRf eRs en IN+ Noiseless IN– eni eno Figure 52. Noise Model The total equivalent input noise density (eni) is calculated by using the following equation: e ni + en 2 ) IN ) R S 2 ) IN– R F ø R G 2 ) 4kTRs ) 4kT RF ø RG Where: k = Boltzmann’s constant = 1.380658 × 10–23 T = temperature in degrees Kelvin (273 + °C) RF || RG = parallel resistance of RF and RG (1) To get the equivalent output noise of the amplifier, just multiply the equivalent input noise density (eni) by the overall amplifier gain (AV). eno + eni AV + eni 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 RF + RG), 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 (RS) and the internal amplifier noise voltage (en). 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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