Lab 4 - EE 420L 

Authored by Hongzhong Li   ,

Today's date: 02/27/2015

Email: lih12@unlv.nevada.edu

NSHE ID: 2000202827

 

Lab description

Op-amps II, gain-bandwidth product and slewing



For the following questions and experiments assume VCC+ = +5V and VCC- = 0V.

 

 
         From the datasheet we know that the unity gain frequency (Fun) is 1.3 MHz
 

 
For Non-Inverting op-amp the bandwidths: BW= Fun/AOL . Therefore:
 
GainsBandwidth(BW)
1 1.3MHz
5260KHz
10130KHz
  
    
When designing the circuit for different gains, we ultilize the formula Av=1+R2/R1 to achieve the desirable gain.
         

Non-Inverting OP-AMP with gain of 1
            Schematic and Simulation
 Experimental   Result

Non-Inverting OP-AMP with gain of 5
Schematic and Simulation
Experimental   Result

Non-Inverting OP-AMP with gain of 10
Schematic and Simulation
Experimental   Result
 

              

            The reason that the simulation bandwidths are higher than the experimental results is because we are only supplying 5V to the op-amp comparing to the 30V specified in the datasheet. If we use a 30V supply voltage we can expect to see better matching result.

 

 
 
For Inverting op-amp the bandwidths: BW= R2/(R1+R2)/abs(-R2/R1) . Therefore:
 
GainsBandwidth(BW)
-1650KHz
-5217KHz
-10118KHz
 

 

Inverting OP-AMP with gain of 1
Schematic and Simulation
Experimental   Result

Inverting OP-AMP with gain of 5
Schematic and Simulation
Experimental   Result

 

Inverting OP-AMP with gain of 10
Schematic and Simulation
Experimental   Result

 

 

 From the datasheet, we can get the following entry shown the slew rate of LM324.

 

 
Using a pulse input signal to measure LM324 slew rate. The circuit and simulation result are shown as below. The output from 10% to 90% is equal to 0.086V and the rise time is approximately 0.448us.The slew rate being defined as the maximum change in voltage per unit time can be calculated by dividing the ouput voltage by the rise time (0.086V/0.448us = 0.192 V/us)



Similiary, we can measure the slew rate using a sinewave input signal. The circuit and simlation result is shown as below.  The slew rate of a sine wave input to the LM324 op-amp is approximately equal to (0.6V/2.904us = 0.2 V/us)
 
 
 For this experiment, we increased our rail to 30 V to prevent our circuit from saturation. The design is implemented using the non-inverting topology. By measuring the rise time and output voltage from 10%-90% we estimate the slew rate. Since the slew rate of a circuit depends on both the amplitude and frequency of the circuit becuase the slew rate can be achieved by increasing one or the other (or both), therefore by increasing both, we can generate the maximumin slew rate with a reasonable input signal.
 

Our measurements are about half of the typical value (0.4V/us) of the datasheet's specifications. This is due to our design not generating enough output swing since the circuit's gain is relatively low. Therefore our slewrate is not as high as the typical value of (0.4 V/us) from the datasheet.

 

Concluson:

From above experiments, I learned the relationship between frequency, close-loop gain, unity-gain frequency and gain-bandwidth product. By studying gain-bandwidth product, we can deisgn circuit using the two methods to measure the slew rate of an op-amp.

 

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