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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>10</strong>.2.2 Noise Floor<br />

<strong>Op</strong> Amp Noise <strong>The</strong>ory and Applications<br />

Characterization<br />

When all <strong>in</strong>put sources are turned off and <strong>the</strong> output is properly term<strong>in</strong>ated, <strong>the</strong>re is a level<br />

of noise called <strong>the</strong> noise floor that determ<strong>in</strong>es <strong>the</strong> smallest signal for which <strong>the</strong> circuit is<br />

useful. <strong>The</strong> objective for <strong>the</strong> designer is to place <strong>the</strong> signals that <strong>the</strong> circuit processes<br />

above <strong>the</strong> noise floor, but below <strong>the</strong> level where <strong>the</strong> signals will clip.<br />

<strong>10</strong>.2.3 Signal-to-Noise Ratio<br />

<strong>The</strong> nois<strong>in</strong>ess of a signal is def<strong>in</strong>ed as:<br />

S (f)<br />

N (f)<br />

<br />

rms signal voltage<br />

rms noise voltage<br />

(<strong>10</strong>–1)<br />

In o<strong>the</strong>r words, it is a ratio of signal voltage to noise voltage (hence <strong>the</strong> name signal-tonoise<br />

ratio).<br />

<strong>10</strong>.2.4 Multiple Noise Sources<br />

When <strong>the</strong>re are multiple noise sources <strong>in</strong> a circuit, <strong>the</strong> total root-mean-square (rms) noise<br />

signal that results is <strong>the</strong> square root of <strong>the</strong> sum of <strong>the</strong> average mean-square values of <strong>the</strong><br />

<strong>in</strong>dividual sources:<br />

ETotalrms e2 1rms e2 2rms e2 <br />

nrms<br />

(<strong>10</strong>–2)<br />

Put ano<strong>the</strong>r way, this is <strong>the</strong> only “break” that <strong>the</strong> designer gets when deal<strong>in</strong>g with noise.<br />

If <strong>the</strong>re are two noise sources of equal amplitude <strong>in</strong> <strong>the</strong> circuit, <strong>the</strong> total noise is not<br />

doubled (<strong>in</strong>creased by 6 dB). It only <strong>in</strong>creases by 3 dB. Consider a very simple case, two<br />

noise sources with amplitudes of 2 V rms:<br />

ETotalrms 22 22 <br />

8 2.83 Vrms<br />

(<strong>10</strong>–3)<br />

<strong>The</strong>refore, when <strong>the</strong>re are two equal sources of noise <strong>in</strong> a circuit, <strong>the</strong> noise is<br />

20 log 2.83<br />

3.01 dB higher than if <strong>the</strong>re were only one source of noise — <strong>in</strong>stead<br />

2<br />

of double (6 dB) as would be <strong>in</strong>tuitively expected.<br />

This relationship means that <strong>the</strong> worst noise source <strong>in</strong> <strong>the</strong> system will tend to dom<strong>in</strong>ate<br />

<strong>the</strong> total noise. Consider a system <strong>in</strong> which one noise source is <strong>10</strong> V rms and ano<strong>the</strong>r is<br />

1 V rms:<br />

ETotalrms <strong>10</strong>2 12 <br />

<strong>10</strong>1 <strong>10</strong>.05 Vrms<br />

<strong>The</strong>re is hardly any effect from <strong>the</strong> 1-V noise source at all!<br />

(<strong>10</strong>–4)<br />

<strong>10</strong>-3

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