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

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

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Ideal <strong>Op</strong> Amp Assumptions<br />

3-2<br />

a hard voltage source such as ground, <strong>the</strong>n <strong>the</strong> o<strong>the</strong>r <strong>in</strong>put is at <strong>the</strong> same potential. <strong>The</strong><br />

current flow <strong>in</strong>to <strong>the</strong> <strong>in</strong>put leads is zero, so <strong>the</strong> <strong>in</strong>put impedance of <strong>the</strong> op amp is <strong>in</strong>f<strong>in</strong>ite.<br />

Fourth, <strong>the</strong> output impedance of <strong>the</strong> ideal op amp is zero. <strong>The</strong> ideal op amp can drive any<br />

load without an output impedance dropp<strong>in</strong>g voltage across it. <strong>The</strong> output impedance of<br />

most op amps is a fraction of an ohm for low current flows, so this assumption is valid <strong>in</strong><br />

most cases. Fifth, <strong>the</strong> frequency response of <strong>the</strong> ideal op amp is flat; this means that <strong>the</strong><br />

ga<strong>in</strong> does not vary as frequency <strong>in</strong>creases. By constra<strong>in</strong><strong>in</strong>g <strong>the</strong> use of <strong>the</strong> op amp to <strong>the</strong><br />

low frequencies, we make <strong>the</strong> frequency response assumption true.<br />

Table 3–1 lists <strong>the</strong> basic ideal op amp assumptions and FIgure 3–1shows <strong>the</strong> ideal op<br />

amp.<br />

Table 3–1. Basic Ideal <strong>Op</strong> Amp Assumptions<br />

IB = 0<br />

VE = 0<br />

IB = 0<br />

Figure 3–1. <strong>The</strong> Ideal <strong>Op</strong> Amp<br />

PARAMETER NAME PARAMETERS SYMBOL VALUE<br />

Input current IIN 0<br />

Input offset voltage VOS 0<br />

Input impedance ZIN ∞<br />

Output impedance ZOUT 0<br />

Ga<strong>in</strong> a ∞<br />

_<br />

+<br />

Zi = ∝<br />

ZO = 0<br />

a = ∝<br />

VOUT

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