Application Division
Description
The CLC420 is a high-speed, slew-boosted, voltage feedback amplifier with unity-gain stability.These features along
with matched inputs, low input bias and noise currents, and
excellent CMRR render the CLC420 very attractive for active
filters, differential amplifiers, log amplifiers, and transimpedance amplifiers.
DC accuracy
Unlike current-feedback amplifiers, voltage-feedback amplifiers have matched inputs. This means that the non-inverting
and inverting input bias current are well matched and track
over temperature, etc. As a result, by matching the resistance looking out of the two inputs, these errors can be reduced to a small offset current term.
Gain bandwidth product
Since the CLC420 is a voltage-feedback op-amp,
closed-loop bandwidth is approximately equal to the
gain-bandwidth product (typically 100MHz) divided by the
noise gain of the circuit (for noise gains greater than 5). At
lower noise gains, higher-order amplifier poles contribute to
higher closed-loop bandwidth. At low gains use the frequency response performance plots given in the data sheet.
Another point to remember is thattheclosed-loop bandwidth
is determined by the noise gain, not the signal gain of the circuit. Noise gain is the reciprocal of the attenuation in the
feedback network enclosing the op amp. For example, a
CLC420 setup as a non-inverting amplifier with a
closed-loop gain of +1 (a noise gain of 1) has a 300MHz
bandwidth. When used as an inverting amplifier with a gain
of −1 (a noise gain of 2), thebandwidth is less, typically only
100MHz.
Full-power bandwidth, and slew-rate
The CLC420 combines exceptional full-power bandwidths
(40MHz, V
0
=
5Vpp, A
v
=
+1) and slew rates (1100V/µs,
A
v
=
+1) with low (40mW) power consumption. These attractive results are achieved by using slew-boosting circuitry to
keep the slew rates high while consuming very little power.
In non-slew boosted amplifiers, full-power bandwidth can be
easily determined from slew-rate measurements, but in
slew-boosting amplifiers, such as the CLC420, you can’t. For
this reason we provide data for both.
Slew rate is also different for inverting and non-inverting configurations. This occurs because common-mode signal voltages are present in non-inverting circuits but absent in inverting circuits. Once again data is provided for both.
DS012752-16
FIGURE 1. Recommended Non-Inverting Gain Circuit
DS012752-17
FIGURE 2. Recommended Inverting Gain Circuit
CLC420
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