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Op Amps for Everyone - The Repeater Builder's Technical ...

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Amplifiers<br />

A.3.2<br />

Inverting <strong>Op</strong> Amp with Inverting Negative Reference<br />

<strong>The</strong> transfer equation takes the <strong>for</strong>m of Y = –mX + b and is given in Equation A–2.<br />

V OUT<br />

V IN<br />

R F<br />

R G1<br />

V REF<br />

R F<br />

R G2<br />

A–2<br />

<strong>The</strong> transfer function slope is negative, and the dc intercept is positive (Figure A–6). R G1<br />

and R G2 are contained in the equation, thus it is easy to obtain the desired slope and dc<br />

intercept by adjusting the value of both resistors. Because of the virtual ground at the inverting<br />

input, R G2 is the terminating impedance <strong>for</strong> V REF . When the reference voltage is<br />

0, the input voltage is constrained to negative voltages because positive input voltages<br />

would cause the output voltage to saturate at ground.<br />

+ 5 V<br />

R G1<br />

R F<br />

V IN<br />

R G2<br />

V REF<br />

+V CC<br />

_<br />

+<br />

V OUT<br />

V OUT — 1 V/Div<br />

– 5 V<br />

– 5 V<br />

V IN — 1 V/Div<br />

+ 5 V<br />

V IN = 10 Vp-p<br />

V REF = –1 V<br />

V CC = 5 V R G1 = R G2 = R F = 10 k<br />

<strong>Op</strong> Amp = TLV247x<br />

Figure A–6. Inverting <strong>Op</strong> Amp with Inverting Negative Reference<br />

A-6

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