Wien Bridge Oscillator and Sawtooth Generator Lab Report, Study Guides, Projects, Research of Electrical and Electronics Engineering

A lab report for ece 3274 students, focusing on the design, implementation, and analysis of a wien bridge oscillator and a sawtooth waveform generator. The report includes schematics, calculations, and experimental results.

Typology: Study Guides, Projects, Research

Pre 2010

Uploaded on 02/13/2009

koofers-user-pin-1
koofers-user-pin-1 🇺🇸

3

(1)

10 documents

1 / 6

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
ECE 3274 LAB 3 Project Sinusoidal Oscillator
Revised: Fall 2008 1 of 6
Project Sinusoidal Oscillator
Objective: This project will demonstrate the basic operation and design of a Wien
bridge RC oscillator.
Components: 741 op-amp, 1N4001 diode (2), 2N7000 MOSFET
Introduction: An oscillator is a circuit that converts a dc input to an ac output. This
project investigates sinusoidal, output oscillators. Sinusoidal oscillators consist of an
amplifier with a positive feedback loop of a frequency selective network. The amplifier
can be a transistor amplifier or an operational amplifier. The frequency of the oscillator
is determined by the frequency selective network. The criteria for an oscillator to
produce sinusoidal oscillations are that the magnitude of the loop gain equal unity and the
phase of the loop gain equal zero at the frequency selected for oscillations.
Av
β
Rload
Av = Non-inverting amplifier
β = positive feedback transfer function
І Loop gain І = І (Av)(β) І = 1
An oscillator with a loop gain of exactly unity is unrealizable because of varying
component values, parameters, and temperatures. To keep the oscillations from ceasing
or increasing, a nonlinear circuit can be used to control the gain and force the loop gain to
remain at unity. The Wien bridge oscillator of Figure 2 uses two diodes in the circuit to
limit the amplitude of the oscillations.
The Wien bridge oscillator without amplitude stabilization is shown in Figure 1.
Wien bridge oscillators are noted for high stability and low distortion. This oscillator
will oscillate at the frequency:
RC
f
2
1
0
When:
2
1
2
R
R
pf3
pf4
pf5

Partial preview of the text

Download Wien Bridge Oscillator and Sawtooth Generator Lab Report and more Study Guides, Projects, Research Electrical and Electronics Engineering in PDF only on Docsity!

Project – Sinusoidal Oscillator

Objective: This project will demonstrate the basic operation and design of a Wien bridge RC oscillator.

Components: 741 op-amp, 1N4001 diode (2), 2N7000 MOSFET

Introduction: An oscillator is a circuit that converts a dc input to an ac output. This project investigates sinusoidal, output oscillators. Sinusoidal oscillators consist of an amplifier with a positive feedback loop of a frequency selective network. The amplifier can be a transistor amplifier or an operational amplifier. The frequency of the oscillator is determined by the frequency selective network. The criteria for an oscillator to produce sinusoidal oscillations are that the magnitude of the loop gain equal unity and the phase of the loop gain equal zero at the frequency selected for oscillations.

Av

β

Rload

Av = Non-inverting amplifier β = positive feedback transfer function І Loop gain І = І (Av)(β) І = 1

An oscillator with a loop gain of exactly unity is unrealizable because of varying component values, parameters, and temperatures. To keep the oscillations from ceasing or increasing, a nonlinear circuit can be used to control the gain and force the loop gain to remain at unity. The Wien bridge oscillator of Figure 2 uses two diodes in the circuit to limit the amplitude of the oscillations.

The Wien bridge oscillator without amplitude stabilization is shown in Figure 1. Wien bridge oscillators are noted for high stability and low distortion. This oscillator will oscillate at the frequency:

RC

f

When:

2 1

R

R

For oscillations to start, the value R 2 /R 1 should be made slightly greater than 2. These relations also hold for the Wien bridge oscillator with amplitude stabilization shown in Figure 2.

C

R

C

V out

R

Wien Bridge Oscillator

R

U

uA

3

2

7

4

6 1

+^5

V+

V-

OUT OS

OS

-15 Vdc

R

+15 Vdc

Figure 1: Wien Bridge Oscillator

Wien Bridge Oscillator with Amplitude Stabilization

10K

C

U

uA

3

2

7

4

6 1

+^5

V+

V-

OUT OS

OS

R

-15 Vdc^ D

V out

10K 10K 10K

C R +15 Vdc

D

Figure 2: Wien Bridge Oscillator with Amplitude Stabilization

  1. What effect will the values of C and R in the sawtooth circuit in figure 3 have on the output waveform? Why does this change the output? What affect does the input square have on the output? Calculate the time constant, and the voltage that the output will reach in 500uS. Run the circuit in PSPICE. Use RD=10K, C=100 nF, VDD=20Vdc, and Vs= 0V to 5V Square wave at 1kHz, use VPULSE for Vs. Use IRF150 for the PSPICE MOSFET device.
  2. Change the input square wave to 750Hz. Calculate the time constant. Calculate the expected voltage peak.
  3. Change the input back to 1khz and now change the C=0.047uF. Calculate the time constant. Calculate the expected peak voltage.

Lab Procedure: Wien bridge oscillator

  1. Construct the Wien bridge oscillator circuit of Figure 1. Use the designed values for the resistors and capacitors: Use 15 V supplies for the op- amp.
  2. Capture the waveform output of the oscilloscope; include the plot in your report. Note any distortion in the output waveform or if oscillations begin to increase without bound. If oscillations do not start, try increasing the ratio R 2 /R 1 to slightly greater than 2.0. This can be done easily if you use the decade resistance box for R 2. If oscillations increase without bound, try getting the ratio R 2 /R 1 closer to exactly 2.
  3. Determine the frequency of the oscillations. What is the peak amplitude of the oscillations? Measure the actual values used for R 1 and R 2.
  4. Now add the amplitude stabilization circuit to construct the Wien bridge oscillator of Figure 2. Be sure to connect the 10 k potentiometer correctly. The 10kΏ potentiometer is located on the large proto board.
  5. Before applying power to the circuit, adjust the pot to the bottom of its range. Turn the power on, and while monitoring the output waveform on the oscilloscope gradually increase the pot setting until sustained oscillations occur. Note the changes in the output waveform amplitude and shape during the pot’s adjustment.
  6. Determine the frequency of the oscillations. What is the peak amplitude of the oscillations? Note any distortion in the output sine wave.

Lab Procedure: Sawtooth Waveform Generator

  1. Construct the sawtooth waveform generator of Figure 3. Use a square wave with an upper limit of 5V and a lower limit of 0V at a frequency of 1 kHz for the input signal. Use VDD = 20 V. To begin with, use RD = 10 k and C = 100 nF. Calculate the time constant and the expected Vout. Observe the changes in the output waveform, as you change component values.
  2. Change the RD =15kΩ C= 100nF calculate the new time constant and the expected Vout.
  3. Change the RD =10kΩ C= 47nF calculate the new time constant and the expected Vout.
  4. Change the RD =10kΩ C= 100nF calculate the new time constant and the expected Vout. Generator frequency= 750Hz

Questions:

  1. Why isn’t an input signal source needed to obtain an output voltage signal?
  2. For both oscillators when does the output waveform distort? Why?
    1. Compare the operation of the two Wien bridge oscillator circuits. Comment on differences and similarities.
    2. In the oscillator with the stabilizing circuit discuss the changes in the output waveform amplitude and shape during the pot’s adjustment.
    3. Compare the stabilized oscillator to the non-stabilized oscillator does the frequency change increase or decrease if the amplitude is saturated or not? Explain why it changes.
    4. What effect does increasing the R have on the sawtooth output waveform? Why?
    5. What effect does decreasing C have on the sawtooth output waveform? Why?
    6. What effect does decreasing the frequency of the input clock have on the sawtooth output waveform? Why?