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/* Changing the Tuning of the Colpitts Oscillator */
{{projectinfo|Tutorial| Designing Low and High Frequency Oscillator Circuits BJT Colpitts Oscillators |TUT12-8.png|In this project, the basic concepts of RF.Spice A/D are demonstrated, you will build and analyze a simple voltage divider is modeled and examinedColpitts oscillator with an LC tank circuit.|
*[[CubeCAD]]Bipolar Junction Transistor*VisualizationParallel LC Resonant Circuit *[[EM.Tempo#Lumped Sources | Lumped Sources]]Oscillation Frequency*[[EM.Tempo#Scattering Parameters and Port Characteristics | S-Parameters]] *[[EM.Tempo#Far Field Calculations in FDTD | Far Fields]] *[[Advanced Meshing in EM.Tempo]] Barkhausen Criterion|All versions|{{download|http://www.emagtech.com/contentdownloads/project-file-download-repository|EMProjectRepo/AnalogLesson10.Tempo zip Analog Lesson 1|[[EM.Cube]] 14.810}} }}
=== What You Will Learn ===
[[File:TUT12-1.png|thumb|400px| The Wien Bridge Oscillator.]] In the first part of this tutorial lesson, you will build a Wien Bridge Oscillator using an LM741 Op-Amp and will analyze its oscillatory behavior. In the second part, you will build and test a high frequency Colpitts oscillator using a parallel resonant LC circuit. The primary objective of this tutorial lesson is to underline the challenges of analyzing oscillator circuits.
== Designing a BJT Colpitts Oscillator ==
[[File:TUT12-6.png|thumb|400px| The Colpitts Oscillator.]]
The following is a list of parts needed for this part of the tutorial lesson:
|-
! scope="row"| C1
| Capacitor
| 100n
|-
! scope="row"| C2 - C3
| Capacitor
| 1n
|-
! scope="row"| C4
| Capacitor
| 27n
|-
! scope="row"| L1
| Inductor
| 1n27u
|-
! scope="row"| Q1
| NPN BJT 2N2222
| beta = 150
|-
! scope="row"| Vin
| Vertical Voltmeter
| N/A
|-
! scope="row"| Vout
| Vertical Voltmeter
| N/A
|-
! scope="row"| Iout
| Horizontal Ammeter
| N/A
|}
To place the transistor part 2N222, open the "'''Parts Bin'''" by selecting the "'''Add Part'''" tab of the "'''Toolbox'''" on the left side panel. By default, the "'''Function'''" tab of the Part Bin is active. This means that parts are sorted based on their function. Open the "'''Active Components'''" menu and select the "'''Transistor...'''" item and from its submenu select the '''NPN...''' item as shown below. All the NPN BJT devices are listed in the Parts Bin. Scroll down the list and find and select “'''2N2222'''”. Either double-click the part's name or click the {{key|Place Part}} button at the bottom of the Parts Bin to place the device on your schematic.
<table><tr><td>[[File:TUT12----6A.png|thumb|650px| Selecting a BJT part in Parts Bin.]] </td></tr></table>
Voltage Source VCCThe figure below shows a Colpitts oscillator: 12V
NPN BJT: 2N2222<table><tr>Four Resistors: R1, R2, R3 and R4<td> Three Capacitors[[File: C1, C2 and C3TUT12-6.png|thumb|570px| The Colpitts Oscillator.]] </td>Inductor: L1</tr> ----</table>
The opposite figure shows a Colpitts oscillator. The parallel resonant LC circuit consisting of L1 and capacitors C3 and C4 is connected between the base and the collector of transistor Q1, and partial feedback voltage is fed to its emitter through the voltage divider constituted by C3 and C4. The oscillating frequency of Colpitts oscillator can be calculated from:
<math>f_o = \frac {1}{2 \pi \sqrt{ L_1 \left( \frac{C_3 C_4}{C_3 + C_4} \right) } }</math>
[[File:TUT12-7.png|thumb|300px400px| The operating point results obtained through DC Bias Test of the Colpitts Oscillator.]]
Note that C1 and C2 are bypass and coupling capacitors, respectively. In this Colpitts oscillator circuit, the feedback factor &beta;(s) is C3/(C3 + C4) &cong; C3/C4. The voltage gain A is given by:
<math>A = g_m R = \frac{I_C}{V_T} R_3 = \frac{kI_C}{qT} R_3</math>
Therefore, the Barkausen Barkhausen criterion can be written as:
<math>A \beta(s) = \left( \frac{C_3}{C_3 + C_4} \right). \left( \frac{I_C}{V_T} \right). R_3 \ge 1</math>
Before running a Transient Test of your Colpitts oscillator, first run a DC Bias Test to find the DC operating point of the BJT. The results of the DC bias test are shown in the opposite figure. According to this table, the quiescent collector current I<sub>C</sub> is 2.985mA. The Barkhausen criterion in this case is thus satisfied:
<math>A \beta(s) = \left( \frac{1nF}{16nF} \right). \left( \frac{2.985e985\times 10^{-3}}{26\times 10^{26e-3}} \right). 2e3 2\times 10^3 = 14.351 \ge 1</math>
Now run a Transient Test of your oscillator circuit with start and stop times set at 0 and 100&mu;s, respectively, and a Step Ceiling equal to 1ns. The output voltage graph is shown in the figure below. The output signal oscillates between 2V and 14V. A signal period of almost 1&mu;s can be measured, which corresponds to an oscillation frequency of 1MHz.
<tr>
<td>
[[File:TUT12-8.png|thumb|800px720px|The output voltage of the Colpitts Oscillator.]]
</td>
</tr>
<tr>
<td>
[[File:TUT12-9.png|thumb|800px720px|The output voltage of the modified Colpitts Oscillator with C3 = 0.25nF and L1 = 6.75&mu;H.]]
</td>
</tr>
<tr>
<td>
[[File:TUT12-10.png|thumb|800px720px|The output voltage of the modified Colpitts Oscillator with C3 = 62.5pF and L1 = 6.75&mu;H.]]
</td>
</tr>
</table>
 
<p>&nbsp;</p>
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