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

[[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:AN23In fig 2c.jpg|thumb|right|250px|Fig. 2c.jpg]][[File:AN23 fig 2d.jpgElectronotes/AN-22|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[[operational Transconductancetransconductance Amplifieramplifier]] (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<math>I_{c}</math>) of ththe 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[[transconductance]]" 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)

We can thus look at the circuit of Fig. la1a as a form of a voltage-controlled resistor. If we rewrite equation (1) a little we get:

where <math>R_{eq} = \frac{23.7}{I_{c}}</math>, and where we have made use of the values shown for the [[voltage divider]] [[attenuator]]. What kind of a VCR is this? Well, we can see that the ground point receives current as though it were being supplied from a voltage <math>V_{in}</math> through a resistor <math>R_{eq}</math> is shown in Fig. lb1b. However, this is not a load resistor since the actual load presented by the VCR is always 100,220 ohms. Thus, it is a resistor from an input as seen from ground. If we consider the standard [[operational amplifier inverter|inverting amplifier]] circuit of Fig. lc1c, which has gain <math>-\frac{R_{f}}{R_{i}}</math>, we can see that if we put this VCR in place of <math>R_{i}</math>, we get the gain control of AN-22 from a different point of view. This is shown in Fig. Id1d. This is a very useful VCR and finds many applications such as in the voltage-controlled [[operational amplifier integrator|integrator]] shown in Fig. le1e. Two of these VC integrators and an [[operational amplifier|op-amp]] [[summer]] can be used to form a VC [[state-variable filter]], which is very useful as a basic voltage-controlled filter block.

Next we would like to look to see if we can make a VCR that looks like a resistive load. That is, we want to have a VCR that actually draws different currents depending on the voltage across it - which after all is what a real resistor does. This can be implemented as shown in Fig. 2a. Ignore for the moment the upper op-amp in Fig. 2a, which is just a [[operational amplifier buffer|voltage follower]] to drive the attenuator on the input of the CA3080. The output of the CA3080 is thus

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|high-pass filter]] structure shown in Fig. 2c. The implementation is shown in Fig. 2d, and the 3dB frequency is <math>\frac{1}{2 \pi R_{eq}C}</math>.

Thus we have implemented three types of VCR's. The first (Fig. la1a) is useful for supplying current to a ground potential. The second (Fig. 2a) is useful as a resistor to ground. The third (using the differential input arrangement of which Fig 3b is an example) is one form of a floating resistor.

Thus, as the current <math>I_{c}</math> is increased, the effective resistance goes down, starting from a value of 200k (or whatever attenuator is used). For a completely linear system, the circuit of Fig. 5 can be used to get rid of the l/<math>\frac{1}{200k}</math> term.

* Electronotes[http://electronotes.netfirms.com/AN23.PDF Application Note No. 23], Electronotes, 18 January 1977, © Bernie Hutchins