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

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Additional Parameter Information<br />

11.3.7.1 Input Capacitance<br />

Input capacitance, Ci, is measured between <strong>the</strong> <strong>in</strong>put term<strong>in</strong>als with ei<strong>the</strong>r <strong>in</strong>put grounded.<br />

Ci is usually a few pF. In Figure 11–5, if Vp is grounded, <strong>the</strong>n Ci = Cd || Cn. Sometimes common-mode <strong>in</strong>put capacitance, Cic is specified. In Figure 11–5, if Vp is<br />

shorted to Vn, <strong>the</strong>n Cic = Cp || Cn. Cic is <strong>the</strong> <strong>in</strong>put capacitance a common mode source<br />

would see referenced to ground.<br />

11.3.7.2 Input Resistance<br />

Input resistance, ri is <strong>the</strong> resistance between <strong>the</strong> <strong>in</strong>put term<strong>in</strong>als with ei<strong>the</strong>r <strong>in</strong>put grounded.<br />

In Figure 11–5, if Vp is grounded, <strong>the</strong>n ri = Rd || Rn. ri ranges from <strong>10</strong>7 Ω to <strong>10</strong>12 Ω, depend<strong>in</strong>g<br />

on <strong>the</strong> type of <strong>in</strong>put.<br />

Sometimes common-mode <strong>in</strong>put resistance, ric, is specified. In Figure 11–5, if Vp is<br />

shorted to Vn, <strong>the</strong>n ric = Rp || Rn. ric is <strong>the</strong> <strong>in</strong>put resistance a common mode source would<br />

see referenced to ground.<br />

11.3.8 Output Impedance<br />

Different data sheets list <strong>the</strong> output impedance under two different conditions. Some data<br />

sheets list closed-loop output impedance while o<strong>the</strong>rs list open-loop output impedance,<br />

both designated by Zo. Zo is def<strong>in</strong>ed as <strong>the</strong> small signal impedance between <strong>the</strong> output term<strong>in</strong>al and ground. Data<br />

sheet values run from 50 Ω to 200 Ω.<br />

Common emitter (bipolar) and common source (CMOS) output stages used <strong>in</strong> rail-to-rail<br />

output op amps have higher output impedance than emitter follower output stages.<br />

Output impedance is a design issue when us<strong>in</strong>g rail-to-rail output op amps to drive heavy<br />

loads. If <strong>the</strong> load is ma<strong>in</strong>ly resistive, <strong>the</strong> output impedance will limit how close to <strong>the</strong> rails<br />

<strong>the</strong> output can go. If <strong>the</strong> load is capacitive, <strong>the</strong> extra phase shift will erode phase marg<strong>in</strong>.<br />

Figure 11–6 shows how output impedance affects <strong>the</strong> output signal assum<strong>in</strong>g Zo is mostly<br />

resistive.<br />

11-14<br />

ZO<br />

AVD RL<br />

Resistive Load<br />

VO<br />

RL VO AVD RL Z 0<br />

Figure 11–6.Effect of Output Impedance<br />

ZO<br />

AVD CL<br />

Capacitive Load<br />

VO<br />

VO <br />

1<br />

jff 0 1<br />

fO <br />

1<br />

Where:<br />

2Z 0C L<br />

Some new audio op amps are designed to drive <strong>the</strong> load of a speaker or headphone directly.<br />

<strong>The</strong>y can be an economical method of obta<strong>in</strong><strong>in</strong>g very low output impedance.

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