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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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12-18<br />

this yields m = 16.16. <strong>The</strong> resistors R1 and R2 are calculated with <strong>the</strong> aid of Equations<br />

12–22 and 12–23.<br />

R 1<br />

R 1 R 2<br />

b<br />

V REF R G<br />

R F R G <strong>10</strong>.4<br />

2.495 23.7<br />

23.7 383 0.2424<br />

R 1 0.2424<br />

0.7576 R 2 0.32 R 2<br />

(12–22)<br />

(12–23)<br />

<strong>The</strong> parallel comb<strong>in</strong>ation of R 1 and R 2 should equal <strong>the</strong> parallel comb<strong>in</strong>ation of R F and<br />

R G so that <strong>the</strong> <strong>in</strong>put voltage offset caused by <strong>the</strong> op amp <strong>in</strong>put current is cancelled. Select<br />

R 2 = <strong>10</strong>5 kΩ and R 1 = 33.2 kΩ because <strong>the</strong>y are standard 1% values, and <strong>the</strong>n b = <strong>10</strong>.3.<br />

<strong>The</strong> value of <strong>the</strong> parallel comb<strong>in</strong>ation of R 1, R 2 (R 1||R 2 = 25.22 kΩ) almost matches <strong>the</strong><br />

value of <strong>the</strong> parallel comb<strong>in</strong>ation of R F, R G (R F||R G = 22.3kΩ), and this is an adequate<br />

match for <strong>in</strong>put current cancellation. <strong>The</strong> downsides of select<strong>in</strong>g large resistor values for<br />

R F are current noise amplification, <strong>in</strong>creased resistor noise, smaller bandwidth because<br />

of stray capacitance, and <strong>in</strong>creased offset voltage due to <strong>in</strong>put current. Bandwidth clearly<br />

is not a factor <strong>in</strong> this design. <strong>The</strong> op amp <strong>in</strong>put current is <strong>10</strong>0 pA, so it won’t cause much<br />

offset with a 383-kΩ feedback resistor (38.3 µV). <strong>The</strong> noise current and voltage are calculated<br />

later when <strong>the</strong> error budget is made.<br />

<strong>The</strong> ga<strong>in</strong>, m, and <strong>the</strong> <strong>in</strong>tercept, b, are not accurate because <strong>the</strong> exact resistor values were<br />

not available <strong>in</strong> <strong>the</strong> 1%-resistor selection chart. This is a normal situation, and <strong>in</strong> less demand<strong>in</strong>g<br />

designs <strong>the</strong> small error ei<strong>the</strong>r does not matter or is corrected someplace else<br />

<strong>in</strong> <strong>the</strong> signal cha<strong>in</strong>. That error is critical <strong>in</strong> this design, so it must elim<strong>in</strong>ated. <strong>The</strong>re are several<br />

nondrift type errors that have accumulated up to this po<strong>in</strong>t, and now is <strong>the</strong> time to correct<br />

all <strong>the</strong> nondrift errors with <strong>the</strong> addition of adjustments. Two adjustments are used; one<br />

adjustment controls <strong>the</strong> ga<strong>in</strong>, m, and <strong>the</strong> o<strong>the</strong>r controls <strong>the</strong> <strong>in</strong>tercept, b. <strong>The</strong> value of <strong>the</strong><br />

adjustable resistor must be large enough to deliver an adequate adjustment range, but<br />

any value larger than that decreases <strong>the</strong> adjustment resolution.<br />

<strong>The</strong> data that determ<strong>in</strong>es <strong>the</strong> adjustment range required is tabulated <strong>in</strong> Table 12–5. Drift<br />

and ga<strong>in</strong> errors are calculated <strong>in</strong> volts, but drift errors are calculated <strong>in</strong> bits because <strong>the</strong>y<br />

are not elim<strong>in</strong>ated by adjustments. Remember, a LSB for this system is 4/4096 =<br />

976.6 µV/bit.

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