Electronotes/AN-23 - The CA3080 as a voltage-controlled resistor: Difference between revisions

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[[File:AN23 fig 1a.jpg|thumb|right|250px|Fig. 1a.jpg]][[File:AN23 fig 1b.jpg|thumb|right|250px|Fig. 1b.jpg]][[File:AN23 fig 1c.jpg|thumb|right|250px|Fig. 1c.jpg]][[File:AN23 fig 1d.jpg|thumb|right|250px|Fig. 1d.jpg]][[File:AN23 fig 1e.jpg|thumb|right|250px|Fig. 1e.jpg]][[File:AN23 fig 2a.jpg|thumb|right|250px|Fig. 2a.jpg]][[File:AN23 fig 2b.jpg|thumb|right|250px|Fig. 2b.jpg]][[File:AN23 fig 2c.jpg|thumb|right|250px|Fig. 2c.jpg]][[File:AN23 fig 2d.jpg|thumb|right|250px|Fig. 2d.jpg]][[File:AN23 fig 3a.jpg|thumb|right|250px|Fig. 3a.jpg]][[File:AN23 fig 3b.jpg|thumb|right|250px|Fig. 3b.jpg]]In AN-22, we looked at the CA3080 Operational Transconductance Amplifier (OTA) as a voltage-controlled gain source. Here, we will use these previous ideas as a jumping-off point to see how the CA3080 can be made to act like a voltage-controlled resistor (VCR). In these applications, the CA3080 is used in its linear mode, so signals at the actual input pins are limited to (generally attenuated to) ±10 mV. In the cases below we will not be showing the actual circuitry that controls the control current (Ic) of th CA3080, but the reader can consider this circuitry to be similar to that shown in AN-22. The fact that the CA3080 could look like a resistor is implied by the name "transconduct ance" and can be seen by writing the basic equation for the CA3080 as:
 
<math>\frac{V_{diff}}{I_{out}} = \frac{1}{(19.2 \cdot I_{c}})</math> (1)
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which is the same thing we had above. But here the current is drawn from the input (<math>I_{in} = I_{out}</math>) so the VCR looks like a resistor to ground, as seen in Fig. 2b. We can thus use this sort of VCR to implement the high-pass filter structure shown in
Fig. 2c. The implementation is shown in Fig. 2d, and the 3dB frequency is <math>\frac{l}{2 \pi R_{eq}C}</math>.
<div><ul>
<li style="display: inline-block;">[[File:AN23 fig 2c.jpg|thumb|right|250px|Fig. 2c.jpg]]</li>
<li style="display: inline-block;">[[File:AN23 fig 2d.jpg|thumb|right|250px|Fig. 2d.jpg]]</li>
<li style="display: inline-block;">[[File:AN23 fig 3a.jpg|thumb|right|250px|Fig. 3a.jpg]]</li>
<li style="display: inline-block;">[[File:AN23 fig 3b.jpg|thumb|right|250px|Fig. 3b.jpg]]</li>
</ul></div>
Since we have implemented the simple R-C high-pass filter (with an output buffer), it is of interest to ask if the corresponding R-C low-pass filter can be realized. It might at first seem that the VCR of Fig. la would be the answer, but if we look at this closely we see that it supplies a current that is indeed proportional to an input voltage, but the other end is always taken to be ground, while in the simple R-C low-pass, the voltage "x" (see Fig. 3a) is not in general zero. Thus, we need a VCR which sees two voltages, <math>V_{in}</math>, and the voltage "x" which is the same as the output voltage. The circuit of Fig. 3b is the proper realization. This is easy to show.
 
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A more general form of a floating resistor is shown in Fig. 4, and is a circuit first suggested by G. Wilcox.
<div><ul>
[[File:AN23 fig 4.jpg|thumb|250px|Fig. 4.jpg]][[File:AN23 fig 5.jpg|thumb|250px|Fig. 5.jpg]]
<li style="display: inline-block;">[[File:AN23 fig 4.jpg|thumb|250px|Fig. 4.jpg]]</li>
[[File<li style="display:AN23 fig 4.jpg|thumb|250px|Fig. 4.jpg]]inline-block;">[[File:AN23 fig 5.jpg|thumb|250px|Fig. 5.jpg]] </li>
</ul></div>
First assume that <math>I_{c}=0</math>, and thus the two CA3080's are effectively out of the circuit. The resulting resistance between <math>V_{1}</math> and <math>V_{2}</math> is just 100k + 100k + 220 which is approximately 200k. Now, if a current <math>I_{c}</math> is flowing in both CA3080's, it can be shown that the current I is given by: