^{o}.

This means that if the input pulse is positive, then the output pulse will be negative and vice versa. The figure below shows an **inverting operational amplifier** built by using an op-amp and two resistors. Here we apply the input signal to the inverting terminal of the op-amp via the resistor R_{i}. We connect the non-inverting terminal to ground. Further, we provide the feedback necessary to stabilize the circuit, and hence to control the output, through a feedback resistor R_{f}.

Mathematically the voltage gain offered by the circuit is given as

Where,

However, we know that an ideal op amp has infinite input impedance due to which the currents flowing into its input terminals are zero i.e. I_{1} = I_{2} = 0. Thus, I_{i} = I_{f}. Hence,

We also know that in an ideal op amp the voltage at inverting and non-inverting inputs are always equal.

As we have grounded the non – inverting terminal, zero voltage appears at the non – inverting terminal. That means V_{2} = 0. Hence, V_{1} = 0, also. So, we can write

From, above two equations, we get,

The voltage gain of the **inverting operational amplifier** or **inverting op amp** is,

This indicates that the voltage gain of the inverting amplifier is decided by the ratio of the feedback resistor to the input resistor with the minus sign indicating the phase-reversal. Further, it is to be noted that the input impedance of the inverting amplifier is nothing but R_{i}.

**Inverting amplifiers** exhibit excellent linear characteristics which make them ideal as DC amplifiers. Moreover, they are often used to convert input current to the output voltage in the form of Transresistance or Transimpedance Amplifiers. Further, these can also be used in audio mixers when used in the form of Summing Amplifiers.