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Op Amp Circuit Experiment: Amplifying Audio Signals with Variable-Gain Amplifiers - Prof. , Lab Reports of Mechanical Engineering

An experiment on using operational amplifiers (op amps) to amplify audio signals. The experiment involves setting up a unity-gain amplifier (buffer) and a variable-gain inverting amplifier. The circuit analysis using two rules and provides a range for the output voltage based on the resistance of the potentiometer. It also mentions some common op amps and their pin-outs, and provides a diagram of the complete circuit.

Typology: Lab Reports

2009/2010

Uploaded on 03/28/2010

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Download Op Amp Circuit Experiment: Amplifying Audio Signals with Variable-Gain Amplifiers - Prof. and more Lab Reports Mechanical Engineering in PDF only on Docsity! ELVIS Experiment #2 – Operational Amplifiers (Op Amps) Introduction: This experiment demonstrates how Op Amps can be used to amplify an audio signal. Two Op Amps will be used. The first will be set up as a unity-gain amplifier (or “buffer”), and the second will be configured as a variable-gain inverting amplifier. This is illustrated in Figure 1. The experiment will show that using a negative gain amplifier for an audio signal is acceptable. The experiment will also demonstrate some problems that can occur when building Op Amp circuits. Buffer Inverter R2 1 kOhm R1 0 - 10 kOhm Vi Vo Figure 1: Op Amp circuit, including a unity gain “buffer” and a variable-gain inverting amplifier. Circuit Analysis: Op Amp circuits are analyzed by using two rules: 1) the voltage at the inverting input terminal is the same as the voltage at the non-inverting input terminal, and 2) the current entering the two input terminals is zero. That is: 1. np vv = 2. 0== np ii To begin with, the output of the buffer amp is the same as its input. Note, however, that the current from the voltage source Vi is zero. The buffer amp effectively isolates the input from the rest of the circuit (which is where it gets its name). The Inverting amp can also be analyzed by following these two rules. The non-inverting input is grounded, so from rule 1 we know that the voltage at the inverting input is also zero. Using rule 2, we can write KCL at the inverting input as 21 ii = . Using this, we can solve for o v : i_1 i_2 io oi v R R v R v R v ii 1 2 21 21 00 !=" ! = ! "= Based on the range of the resistance of the potentiometer, the output voltage will be between –0.1 and (– !) times the input voltage. Normally, the variable resistor would be 2 R , and the fixed resistor would be 1 R , so that the output voltage would vary between 0 and –10 times the input voltage. For this demonstration, we are intentionally reversing the resistors so that we can create a very large gain and force the op amp outside of its linear range. Implementation: Op Amps are commonly purchased as integrated circuits. A few Op Amp integrated circuits are shown in Figure 2, below. Figure 2: Some common Op Amps The 741 is probably the most common Op Amp, and has become so popular that several competing types have adopted the same configuration of input and output pins, or “pin-out.” The 741’s pin-out is shown below. For this experiment we will use pins 2, 3, 4, 6, and 7 on each of the Op Amp chips. Figure 3: 741 pin-out
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