Imagine that you work in the company “ HHN Mechatronics & Robotics”, which is a cheap mobile EKG – So you want to build a measuring device for the electrocardiogram or the cardiac voltage curve - for athletes and those in need. The measurement signal has only a few millivolts and microamps. In order to protect the signal from electromagnetic radiation on the way from the glued-on electrode to the evaluation electronics, a electromagnetic shielding placed around the line (see figure 1, above). However, since this creates a parasitic capacitor, a colleague suggested active shielding. The shielding is always kept at the measuring voltage that is applied to the line via a voltage follower (see figure 1, under). The parasitic capacitor is never charged due to this structure, since the same voltage prevails on both sides - there is no falsification of the signal. It is important for the application that the voltage follower reacts quickly.

You are supervised with the design of this voltage follower and should use the available operational amplifiers $LM318$, $uA741$ and $uA776$ analyze in the voltage follower circuit.

Write a short report (problem description, circuit in TINA TI, results, discussion) and use TINA TI for the solution.

1. Recreate the circuit described above for a realistic operational amplifier in Tina. Use a voltage generator as a source unit step with the amplitude $U_A = 1.0 V$ .
2. Simulate over Analysis»Transient… the time course for the specified operational amplifiers.
   Determine the time that elapses until the initial value of $0.1 V$ for the first time $0.9 V$ achieved ($10%$ to $90%$ of the amplitude, too. It is called rise time).
3. Describe the passage of time in each case. Are there any other differences besides the rise time?
4. Based on the information provided, which of the three op amps would you choose for the problem?

In-depth information (not relevant for the homework):

• Paper on the Stability of Shield-Driver Circuits
• Detailed description of a EMG/EKG Vorverstärkerschaltung

For the inverting amplifier, derive the voltage gain. Use the procedure that was used for the non-inverting amplifier.
Take into account that for the differential gain $A_D$ of the ideal OPV applies: $A_D \rightarrow \infty$.
This also applies: $1/A_D \rightarrow 0$ , but it doesn't always apply ${{C}\over{U_x \cdot A_D}} \rightarrow 0$, for an unknown constant $C$ and a voltage $U_x$!

• What is looking for?
• Number of variables?
• Number of necessary equations?
• Establishing the known equations
• Derivation of the voltage gain
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  

Which type of amplifier (inverting or non-inverting amplifier) has the lower input resistance? Why?

Below you will find circuits with an ideal operational amplifier, which are similar to the non-inverting amplifier and whose voltage gain $A_V$ must be determined.

Assumptions

• $R_1 = R_3 = R_4 = R$
• $R_2 = 2 \cdot R$
• $U_I$ comes from a low-resistance source
• $U_O$ is due to a high-resistance consumer

Exercises

1. Enter the voltage gain $A_V$ for each circuit. A detailed calculation as before is not necessary.
2. For Figure 7, indicate how the voltage gain can be determined.
3. Generalize with justification how
   1. a short circuit of the two OPV inputs must be taken into account,
   2. Resistances are to be considered when doing this:
      1. with a terminal (“on one side”) are directly and exclusively on an OPV input,
      2. with one terminal each are directly connected to an OPV input.
4. In which circuits do resistors $R_3$ and $R_4$ represent an unloaded voltage divider?

In order to approach the problems, you should try to use the knowledge from the inverting amplifier. It can be useful to simulate the circuits via Falstad-Circuit or Tina TI. In the first two circuits, tips can be seen under the illustration as support.

Important : As always in your studies, you should try to generalize the knowledge gained from the task.