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These two resistors are providing required feedback to the op-amp. In an ideal condition, the input pin of the op-amp will provide high input impedance and the output pin will be in low output impedance. The amplification is dependent on those two feedback resistors R1 and R2 connected as the voltage divider configuration.
Due to this, and as the Vout is dependent on the feedback network, we can calculate the closed loop voltage gain as below. Also, the gain will be positive and it cannot be in negative form. The gain is directly dependent on the ratio of Rf and R1. Now, Interesting thing is, if we put the value of feedback resistor or Rf as 0, the gain will be 1 or unity. And if the R1 becomes 0, then the gain will be infinity. But it is only possible theoretically.
In reality, it is widely dependent on the op-amp behavior and open-loop gain. Op-amp can also be used two add voltage input voltage as summing amplifier. Practical Example of Non-inverting Amplifier We will design a non-inverting op-amp circuit which will produce 3x voltage gain at the output comparing the input voltage. We will make a 2V input in the op-amp.
We will configure the op-amp in noninverting configuration with 3x gain capabilities. We selected the R1 resistor value as 1. R2 is the feedback resistor and the amplified output will be 3 times than the input. Voltage Follower or Unity Gain Amplifier As discussed before, if we make Rf or R2 as 0, that means there is no resistance in R2, and Resistor R1 is equal to infinity then the gain of the amplifier will be 1 or it will achieve the unity gain.
As there is no resistance in R2, the output is shorted with the negative or inverted input of the op-amp. As the gain is 1 or unity, this configuration is called as unity gain amplifier configuration or voltage follower or buffer. As we put the input signal across the positive input of the op-amp and the output signal is in phase with the input signal with a 1x gain, we get the same signal across amplifier output.
Thus the output voltage is the same as the input voltage. So, it will follow the input voltage and produce the same replica signal across its output. This is why it is called a voltage follower circuit. The input impedance of the op-amp is very high when a voltage follower or unity gain configuration is used. Sometimes the input impedance is much higher than 1 Megohm.
So, due to high input impedance, we can apply weak signals across the input and no current will flow in the input pin from the signal source to amplifier. For this reason, the value of the resistor connected at the input must be chosen accordingly. This further creates other problems in the circuit. It can be overcome by the non-inverting amplifiers. What is a Non-Inverting Amplifier?
The amplifier in which the input signal is applied to the non —inverting terminal so that the output obtained is non-inverted. It is similar to that of the inverting amplifier. The same parts of the inverting amplifier are utilized in this amplifier. The only design criteria that must be chosen is that the non-inverting amplifier must possess the high value of the impedance at the input.
Circuit Diagram The non-inverting amplifier are designed using an the operational amplifier. In the op-amps there are three basic terminals among those three two will be the input terminals and one is for output consideration. The applied input to the respective terminal decides whether it is an inverting one or non-inverting one.
The circuit designed for a non-inverting amplifier consists of a basic op-amp where the input is connected to a non-inverting terminal. The output obtained from this circuit is a non-inverted one. This is again feedback towards input but to the inverting terminal via a resistor. Further, one more resistor is connected to the inverting terminal in concern to connect it to the ground.
Hence the overall gain of the circuit is dependent on these two resistors that are responsible for the feedback connection. Those two resistors will behave as a voltage divider of the feedback fed to the inverting terminal. Generally R2 is chosen to be greater than the R1.
Non-Inverting Operational Amplifier Circuit Non-Inverting Amplifier Gain As already discussed the constructional view of the non-inverting amplifier it can be considered that the inputs applied at both the terminals are the same. The voltage levels are the same and even the feedback is dependent on both the resistors R1 and R2. In this way, it makes simple and easy to determine the gain for such types of amplifiers. As the voltage levels applied for both the terminals remain the same indirectly results in the gain levels to be high.
The voltage level determined at the inverting terminal is because of the presence of the potential-divider circuit. Then this results in the equation of the voltage that is: But the gain is the ratio between the ratios of the output values to input values of the applied signals. Therefore, Av represents the overall gain obtained in the circuit. R1 represents the resistance connected to the ground. R2 represents the resistor connected to the feedback.
The resistance considered in the above equation is in ohms.
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