Intro to Operational Amplifiers (Op-Amps)

Operational amplifiers, commonly known as op-amps, are one of the most widely used building blocks in analog electronics. They can amplify weak electrical signals, perform mathematical operations such as addition and subtraction, and serve as the foundation of countless circuits, from audio amplifiers to filters and oscillators.

What is an Operational Amplifier?

An operational amplifier is an integrated circuit (IC) with two input terminals and one output:

Op-amps are called “operational” amplifiers because, in early analog computers, they were designed to perform mathematical operations like addition, subtraction, integration, and differentiation.

Ideal Op-Amp Assumptions

Before diving into real-world circuits, we first consider the ideal op-amp model. In this idealized version, several assumptions simplify analysis:

Although no real op-amp meets these assumptions perfectly, many modern op-amps (like the LM741, TL081, or modern rail-to-rail op-amps) come close enough that we can use the ideal model for most calculations.

The Inverting Amplifier

The inverting amplifier configuration is one of the most common uses of an op-amp. In this circuit, the input signal is applied to the inverting terminal through a resistor, while the non-inverting terminal is grounded.

Deriving the Gain Equation

  1. The voltage at the non-inverting input (+) is 0V (grounded).
  2. By the virtual short principle, the inverting input (–) is also at 0V (virtual ground).
  3. No current flows into the op-amp input, so the input current flows entirely through the feedback resistor.

By Ohm’s Law:

Iin = Vin / Rin

This same current flows through the feedback resistor (Rf):

If = –Vout / Rf

Equating the two currents:

Vin / Rin = –Vout / Rf

Therefore, the gain is:

Vout / Vin = –Rf / Rin

The negative sign indicates that the output is inverted relative to the input.

The Non-Inverting Amplifier

The non-inverting amplifier is another essential configuration. In this setup, the input signal is applied directly to the non-inverting input (+), while the inverting input (–) receives feedback from the output through a resistor divider network.

Deriving the Gain Equation

The voltage at the inverting input is determined by the resistor divider:

V– = (Rin / (Rin + Rf)) × Vout

Since the op-amp forces the inputs to be equal (ideal assumption):

Vin = V–

Rearranging gives:

Vout / Vin = 1 + (Rf / Rin)

This equation shows that the non-inverting amplifier has a positive gain, and the output is in-phase with the input.

Practical Considerations

Real op-amps deviate from the ideal model. Some important non-ideal characteristics include:

Despite these limitations, op-amps remain incredibly useful and versatile in electronics design.

Applications of Op-Amps

Practice Problems

Problem 1: In an inverting amplifier, Rin = 10kΩ and Rf = 100kΩ. What is the gain?

Gain = –Rf / Rin = –100k / 10k = –10

Problem 2: In a non-inverting amplifier, Rin = 5kΩ and Rf = 20kΩ. What is the gain?

Gain = 1 + (Rf / Rin) = 1 + (20k / 5k) = 5

Problem 3: If an inverting amplifier has Rin = 1kΩ and Rf = 47kΩ, and Vin = 0.2V, what is Vout?

Gain = –Rf / Rin = –47. Vout = Gain × Vin = –47 × 0.2V = –9.4V

Conclusion

Operational amplifiers are fundamental to analog electronics. By understanding their ideal behavior and how feedback shapes inverting and non-inverting amplifier circuits, you gain the tools to analyze and design a wide range of circuits. While real op-amps introduce practical limitations, the core principles remain powerful and widely applicable. Keep practicing problems, experiment in simulation tools, and apply these concepts in real circuits to deepen your knowledge.

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