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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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<strong>The</strong> Frequency Characteristics of Passive Components<br />

17.4.2 Capacitors<br />

17-12<br />

High-frequency performance of capacitors is approximated by <strong>the</strong> schematic shown <strong>in</strong><br />

FIgure 17–7.<br />

Figure 17–7. Capacitor High-Frequency Performance<br />

RP<br />

L ESR<br />

C<br />

Capacitors are used <strong>in</strong> analog circuitry for power supply decoupl<strong>in</strong>g and as filter components.<br />

For an ideal capacitor, reactance decreases by <strong>the</strong> formula:<br />

X C 1<br />

(2fC)<br />

Where:<br />

XC capacitive reactance <strong>in</strong> Ohms<br />

F frequency <strong>in</strong> Hz<br />

C capacitance <strong>in</strong> microfarads<br />

(17–1)<br />

<strong>The</strong>refore, a <strong>10</strong>-µF electrolytic capacitor has a reactance of 1.6 Ω at <strong>10</strong> kHz, and 160-µΩ<br />

at <strong>10</strong>0 MHz. Right?<br />

In reality, one will never see <strong>the</strong> 160 µΩ with <strong>the</strong> electrolytic capacitor. Film and electrolytic<br />

capacitors have layers of material wound around each o<strong>the</strong>r, which creates a parasitic<br />

<strong>in</strong>ductance. Self-<strong>in</strong>ductance effects of ceramic capacitors are much smaller, giv<strong>in</strong>g <strong>the</strong>m<br />

a higher operat<strong>in</strong>g frequency. <strong>The</strong>re is also some leakage current from plate to plate,<br />

which appears as a resistance <strong>in</strong> parallel with <strong>the</strong> capacitor, as well as resistance with<strong>in</strong><br />

<strong>the</strong> plates <strong>the</strong>mselves, which add a parasitic series resistance. <strong>The</strong> electrolyte itself <strong>in</strong><br />

electrolytic capacitors is not perfectly conductive (to reduce leakage current). <strong>The</strong>se resistances<br />

comb<strong>in</strong>e to create <strong>the</strong> equivalent series resistance (ESR). <strong>The</strong> capacitors used<br />

for decoupl<strong>in</strong>g should be low ESR types, as any series resistance limits <strong>the</strong> effectiveness<br />

of <strong>the</strong> capacitor for ripple and noise rejection. Elevated temperatures also severely <strong>in</strong>crease<br />

ESR, and can be permanently destructive to capacitors. <strong>The</strong>refore, if an alum<strong>in</strong>um<br />

electrolytic will be subjected to high temperatures, use <strong>the</strong> high-temperature grade<br />

(<strong>10</strong>5C), not <strong>the</strong> low temperature grade (85C).<br />

For leaded parts, <strong>the</strong> leads <strong>the</strong>mselves also add a parasitic <strong>in</strong>ductance. For small values<br />

of capacitance, it is important to keep <strong>the</strong> lead lengths short. <strong>The</strong> comb<strong>in</strong>ation of parasitic<br />

<strong>in</strong>ductance and capacitance can produce resonant circuits! Assum<strong>in</strong>g a lead self-<strong>in</strong>ductance<br />

of 8 nH/cm (see <strong>the</strong> follow<strong>in</strong>g paragraphs), a 0.01-µF capacitor with two 1-cm leads<br />

will resonate at 12.5 MHz. This effect was well known to eng<strong>in</strong>eers many decades ago,

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