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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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Voltage Divider Rule<br />

source, through a component, or through a wire, because all currents are treated identically.<br />

Kirchoff’s current law is illustrated <strong>in</strong> Figure 2–4 and Equations 2–4 and 2–5.<br />

Figure 2–4. Kirchoff’s Current Law<br />

2.3 Voltage Divider Rule<br />

I1<br />

I IN I OUT<br />

I 1 I 2 I 3 I 4<br />

I4 I3<br />

I2<br />

Review of Circuit <strong>The</strong>ory<br />

(2–4)<br />

(2–5)<br />

When <strong>the</strong> output of a circuit is not loaded, <strong>the</strong> voltage divider rule can be used to calculate<br />

<strong>the</strong> circuit’s output voltage. Assume that <strong>the</strong> same current flows through all circuit elements<br />

(Figure 2–5). Equation 2–6 is written us<strong>in</strong>g Ohm’s law as V = I (R 1 + R 2). Equation<br />

2–7 is written as Ohm’s law across <strong>the</strong> output resistor.<br />

Figure 2–5. Voltage Divider Rule<br />

I <br />

V R2<br />

V<br />

R 1 R 2<br />

V OUT IR 2<br />

I<br />

R1<br />

I<br />

VO<br />

(2–6)<br />

(2–7)<br />

Substitut<strong>in</strong>g Equation 2–6 <strong>in</strong>to Equation 2–7, and us<strong>in</strong>g algebraic manipulation yields<br />

Equation 2–8.<br />

V OUT V<br />

R 2<br />

R 1 R 2<br />

(2–8)<br />

A simple way to remember <strong>the</strong> voltage divider rule is that <strong>the</strong> output resistor is divided by<br />

<strong>the</strong> total circuit resistance. This fraction is multiplied by <strong>the</strong> <strong>in</strong>put voltage to obta<strong>in</strong> <strong>the</strong> out-<br />

2-3

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