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AN-6605 Datasheet(PDF) 2 Page - Fairchild Semiconductor |
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AN-6605 Datasheet(HTML) 2 Page - Fairchild Semiconductor |
2 / 5 page AN-6605 APPLICATION NOTE © 2014 Fairchild Semiconductor Corporation www.fairchildsemi.com Rev. 1.0 • 6/25/15 2 1 2 n VEQ= (A12V +A22V ++An2V )1/2 (4) Where VEQ = equalized source noise (V) and An = magnitude of the equalized gain at the center of each noise band (V/V). SOURCE NOISE Models are needed for capacitive and inductive systems such that noise calculations can be made. Namely, the real part of the impedance needs to be determined. A lumped model of a capacitive source, such as condenser or electret microphone, consists of the microphone and stray capacitance shunted by a load resistance. Figure 2. Lumped Model of a Capacitive Microphone It should be noted that for any particular microphone, the noise of the network ((Cm + Cs)//RL) is reduced by increasing RL because Re(Z) (the real part of the impedance) is inversely proportional to RL (see equation 5). The inductive source (phono cartridges and tape heads) is more complex to analyze because it has a much more complex model. The simplified lumped model of a phono cartridge or tape head consists of a series inductance and resistance shunted by a small capacitor. Each phono cartridge or tape head has a recommended load consisting of a specified shunt resistance and capacitance. A model for the inductive source and preamp input network is shown in Figure 3. Figure 3. Phono Cartridge or Tape Head and Preamp Input Network This circuit is quite formidable to analyze and needs, further simplification. Through the use of Q equations, a series L-R is transformed to a parallel L-R. Simplifying the input network to: Figure 4. Simplified Inductive Source Network. |
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