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

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Input Common-Mode Range<br />

18-<strong>10</strong><br />

V<br />

µ<br />

– Input Offset Voltage –<br />

V IO<br />

<strong>10</strong>0<br />

80<br />

60<br />

40<br />

20<br />

0<br />

–20<br />

–40<br />

–60<br />

–80<br />

–<strong>10</strong>0<br />

0 0.5 1 1.5 2 2.5 3<br />

TLV245X<br />

VCC =5 V<br />

TA = 25° C<br />

3.5 4<br />

VIC – Common-Mode Input Voltage – V<br />

4.5 5<br />

Figure 18–6. Input Offset Voltage Changes with Input Common-Mode Voltage<br />

When both transistors are conduct<strong>in</strong>g current <strong>the</strong> <strong>in</strong>put bias currents have a tendency to<br />

cancel, so <strong>in</strong> <strong>the</strong> range of ±1 V, <strong>the</strong> bias current is extremely low even when bipolar transistors<br />

are used to make <strong>the</strong> op amp. Above this range, <strong>the</strong> PNP differential amplifier cuts<br />

off so <strong>the</strong> full bias current requirement of <strong>the</strong> NPN transistor becomes apparent. <strong>The</strong> same<br />

action happens below this range when <strong>the</strong> NPN differential amplifier cuts off. Notice that<br />

<strong>the</strong> PNP bias current is significantly larger than <strong>the</strong> NPN bias current; this is expected because<br />

NPN transistors have better ga<strong>in</strong> characteristics than PNP transistors. <strong>The</strong> baseemitter<br />

voltage of <strong>the</strong> NPN and PNP transistors is well matched because <strong>the</strong> magnitude<br />

of <strong>the</strong> <strong>in</strong>put offset voltage at <strong>the</strong> extremes is almost equal.<br />

<strong>The</strong> bias current and offset voltage variation with <strong>in</strong>put signal amplitude cause errors and<br />

distortion of <strong>the</strong> <strong>in</strong>put signal. Insert<strong>in</strong>g a resistance equal to <strong>the</strong> parallel comb<strong>in</strong>ation of<br />

R F and R G <strong>in</strong>to <strong>the</strong> positive op amp lead m<strong>in</strong>imizes <strong>the</strong> effect of <strong>in</strong>put bias current. <strong>The</strong><br />

resistor, R P, has <strong>the</strong> same voltage drop across it that <strong>the</strong> parallel comb<strong>in</strong>ation of R F and<br />

R G has, hence <strong>the</strong> bias current is converted to a common-mode voltage. <strong>The</strong> commonmode<br />

voltage is normally <strong>in</strong> <strong>the</strong> µV-range because I IB is <strong>in</strong> <strong>the</strong> fractional nA range and R P<br />

is <strong>in</strong> <strong>the</strong> tens of KΩ. <strong>The</strong> CMMR is approximately 60 dB, so <strong>the</strong> <strong>in</strong>put bias current effect<br />

is reduced to <strong>the</strong> nV range where it is <strong>in</strong>significant compared to <strong>the</strong> offset voltage. <strong>The</strong><br />

<strong>in</strong>put offset current is multiplied by R P, and it shows up as an <strong>in</strong>put error. If <strong>the</strong> design can’t<br />

tolerate <strong>the</strong>se errors it is wise to switch to a CMOS op amp because its <strong>in</strong>put currents are<br />

<strong>in</strong> <strong>the</strong> pA range.<br />

Ano<strong>the</strong>r type of error creeps <strong>in</strong> when complementary differential amplifiers are used to<br />

obta<strong>in</strong> DR, and this error is results from <strong>the</strong> different ga<strong>in</strong> of <strong>the</strong> PNP and NPN transistors.

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