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"Chapter 1 - The Op Amp's Place in the World" - HTL Wien 10

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Dynamic Range<br />

18-4<br />

VIN<br />

VnR<br />

Figure 18–1. <strong>Op</strong> Amp Error Sources<br />

V OUT(MIN) <br />

RS<br />

IIB+<br />

IIB–<br />

In<br />

IIO VIB<br />

In<br />

Vn<br />

VCC+ ±∆V<br />

<strong>The</strong> error sources are taken <strong>in</strong>to account <strong>in</strong> Equation 18–3, and this equation refers <strong>the</strong>m<br />

to <strong>the</strong> op amp output by multiply<strong>in</strong>g <strong>the</strong>m by <strong>the</strong> op amp’s closed loop ga<strong>in</strong>.<br />

GCLVIO IIORS VIO T VIN IIBRP <br />

V<br />

Vn InR<br />

CMRR k EQ InRR SVR<br />

+<br />

_<br />

R2<br />

R1<br />

VO<br />

(18–3)<br />

<strong>The</strong> maximum DR that can be achieved by an op amp is given <strong>in</strong> Equation 18–4.<br />

DR 20 Log (18–4)<br />

<strong>10</strong>VOH(MIN) VOL(MAX) VOUT(MAX) 20 Log<br />

V <strong>10</strong><br />

OUT(MIN)<br />

VOUT(MIN) <strong>The</strong> DR is reduced by <strong>the</strong> sum of <strong>the</strong> error terms, so it is proper to conclude that <strong>the</strong> maximum<br />

power supply voltage and <strong>the</strong> op amp choice (this def<strong>in</strong>es <strong>the</strong> error magnitude) both<br />

establish <strong>the</strong> DR of an op amp. <strong>The</strong> first two terms <strong>in</strong> Equation 18–3 are dc error terms,<br />

thus, <strong>the</strong>y can be adjusted to zero by one of several methods not mentioned here. <strong>The</strong><br />

<strong>in</strong>put offset current and <strong>in</strong>put bias current error terms were big factors with older generation<br />

ICs, but today’s technology render <strong>the</strong>m much less significant (see Table 18–1).

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