Difference between revisions of "RF Tutorial Lesson 11: Designing a Microstrip MESFET Amplifier"

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Create two text files as indicated in the tables above. Open [[RF.Spice]]'s Device Editor and select "Create New RF Device from S-Parameter Test File..." from its RF Menu. Follow the program's prompts step by step and create your new RF BJT and MESFET devices.   
 
Create two text files as indicated in the tables above. Open [[RF.Spice]]'s Device Editor and select "Create New RF Device from S-Parameter Test File..." from its RF Menu. Follow the program's prompts step by step and create your new RF BJT and MESFET devices.   
 
 
== Amplifier Design for Maximum Gain==
 
 
[[File:RF142.png|thumb|570px|A general transistor amplifier circuit.]]
 
In this part of the tutorial lesson, you will design an RF amplifier using your MyRFBJT device for maximum gain through conjugate matching. The opposite figure shows the block diagram for a general transistor amplifier. The input and output reflection coefficients are given by:
 
 
 
<math> \Gamma_{in} = \frac{Z_{in} - Z_0}{Z_{in} + Z_0} = s_{11} + \frac{ s_{12}s_{21} \Gamma_L }{1 - s_{22} \Gamma_L} </math>
 
 
 
<math> \Gamma_{out} = \frac{Z_{out} - Z_0}{Z_{out} + Z_0} = s_{22} + \frac{ s_{12}s_{21} \Gamma_S }{1 - s_{11} \Gamma_S} </math>
 
 
 
where &Gamma;<sub>S</sub> and &Gamma;<sub>L</sub> are the source and load reflection coefficients as defined in Tutorial Lesson 6. 
 
 
 
The maximum power transfer will be achieved under conjugate matching conditions at the input and output of the transistor:
 
 
 
<math> \Gamma_S^{\ast} = s_{11} + \frac{ s_{12}s_{21} \Gamma_L }{1 - s_{22} \Gamma_L} </math>
 
 
 
<math> \Gamma_L^{\ast} = s_{22} + \frac{ s_{12}s_{21} \Gamma_S }{1 - s_{11} \Gamma_S} </math>
 
 
 
The above equations can be solved for &Gamma;<sub>S</sub> and &Gamma;<sub>L</sub> as follows:
 
 
 
<math> \Gamma_S = \frac{ B_1 \pm \sqrt{B_1^2-4|C_1|^2} }{2C_1} </math>
 
 
 
<math> \Gamma_L = \frac{ B_2 \pm \sqrt{B_2^2-4|C_2|^2} }{2C_2} </math>
 
 
 
where
 
 
 
<math> B_1 = 1 + |s_{11}|^2 - |s_{22}|^2 - |\Delta |^2  </math>
 
 
 
<math> B_2 = 1 + |s_{22}|^2 - |s_{11}|^2 - |\Delta |^2  </math>
 
 
 
<math> C_1 = s_{11} - \Delta s_{22}^{\ast}  </math>
 
 
 
<math> C_2 = s_{22} - \Delta s_{11}^{\ast}  </math>
 
 
 
<math> \Delta  = s_{11}s_{22} - s_{12}s_{21} </math>
 
 
 
The maximum transducer gain of the amplifier under the conjugate match conditions is given by:
 
 
 
<math> G_{Tmax} = G_S . G_0 . G_L = \frac{1}{1-|\Gamma_S|^2} . |S_{21}|^2 . \frac{1-|\Gamma_L|^2}{\left| 1-s_{22} \Gamma_L \right|^2} </math>
 
 
 
Recalling the definition of the K-parameter from the previous tutorial lesson:
 
 
 
<math> K  = \frac {1 - |s_{11}|^2 - |s_{22}|^2 + |\Delta |^2 } { 2|s_{12}s_{21}| } </math>
 
 
 
one can show that for an unconditionally stable transistor (K > 1), the maximum transducer gain of the amplifier can be written as:
 
 
 
 
<math> G_{Tmax} = \frac{|S_{21}|}{|S_{12}|} \left( K - \sqrt{K^2-1} \right) </math>
 
 
 
== Building a Distributed RF BJT Amplifier==
 
 
[[File:RF145.png|thumb|640px|The distributed RF BJT Amplifier with generic T-Line components.]]
 
[[File:RF144.png|thumb|400px|The property dialog of the imported FR BJT.]]
 
 
The following is a list of parts needed for this part of the tutorial lesson:
 
 
----
 
 
AC Voltage Source: VS (keyboard shortcut: Alt+V)
 
 
Two 50&Omega; Resistors: RS and RL
 
 
RF BJT: MyRFBJT (imported model)
 
 
Two Generic T-Line Segments: T1 and T2 (keyboard shortcut: T)
 
 
Two Generic T-Line Open Stubs: XTLS1 and XTLS2
 
 
Two Ammeters: AM1 and AM2 (keyboard shortcut: Alt+Y)
 
 
Two Net Markers: IN and OUT (keyboard shortcut: Alt+N)
 
 
----
 
 
 
The goal is to design a distributed BJT amplifier for maximum gain at f = 4GHz. From the S-parameter data of the RF BJT at 4GHz, you find that
 
 
 
&Delta; = 0.488 &ang;-162&deg;
 
 
K = 1.195
 
 
&Gamma;<sub>S</sub> = 0.872 &ang;123&deg;
 
 
&Gamma;<sub>L</sub> = 0.876 &ang;61&deg;
 
 
G<sub>Tmax</sub> = 16.7dB;
 
 
 
The input and output matching networks for this project both consist of a generic 50&Omega; T-Line segment together with a shunt generic 50&Omega; T-Line Open Stub as shown in the figure. The lengths of the T-Line Segments and Open Stubs can be found using the same procedure you followed in Tutorial Lesson 3 for stub matching. Given &lambda;<sub>0</sub> = 75mm at f<sub>0</sub> 4GHz, these lengths are found to be:
 
 
{| class="wikitable"
 
|-
 
! T-Line Component !! Z0 !! Electrical Length !! Physical Length at 4GHz
 
|-
 
| T1 || 50&Omega; || 0.120&lambda;<sub>0</sub> || 9mm 
 
|-
 
| XTLOS1 || 50&Omega; || 0.206&lambda;<sub>0</sub> || 19mm 
 
|-
 
| T2 || 50&Omega; || 0.206&lambda;<sub>0</sub> || 19mm 
 
|-
 
| XTLOS2 || 50&Omega; || 0.206&lambda;<sub>0</sub> || 19mm 
 
|-
 
|}
 
 
 
 
[[File:RF148.png|thumb|500px|The distributed RF BJT Amplifier without the source and load sections for the purpose of network analysis.]]
 
 
Place and connect all the parts as shown in the above figure. First, remove the AC voltage source and the source and load resistors to perform network analysis. Run a Network Analysis Test of this circuit with start and stop frequencies set at 3GHz and 5GHz, respectively, with a linear frequency step size of 10MHz. Plot the S-[[parameters]] on an amplitude-only Cartesian graph. The figure below shows the results for s11, s21, s12 and s22 [[parameters]]. It can be seen that the amplifier has a reasonably good return loss at 4GHz. Note that your original S-parameter model of the RF BJT has data for only thee frequencies.
 
 
 
{{Note|[[RF.Spice]] interpolates between a model's available frequency data points to calculate the S-[[parameters]] at all the intermediate frequencies. Therefore, a larger number of measured frequency data points leads to more accurate simulation results.}} 
 
 
 
{| border="0"
 
|-
 
| valign="bottom"|
 
[[File:RF147.png|thumb|900px|left|The graph of magnitude of s11, s21, s12 and s22 parameters of the distributed BJT amplifier circuit.]]
 
|-
 
|}
 
 
 
Next, connect the AC voltage source and the source and load resistors and place the source and load ammeters in a similar manner as in the last part of the previous tutorial lesson. Similarly, define a custom output plot called G<sub>P</sub> for the power gain of your amplifier. Use the same definition: G<sub>P</sub> = 20*log10(abs(i(am2)/i(am1))). Run an AC Frequency Sweep Test of your amplifier from 3GHz to 5GHz with linear frequency steps of 10MHz. The figure below shows the graph of power gain vs. frequency.
 
 
 
{| border="0"
 
|-
 
| valign="bottom"|
 
[[File:RF149.png|thumb|900px|left|The graph of the power gain of the distributed BJT amplifier vs. frequency.]]
 
|-
 
|}
 
 
  
 
== Building a Distributed MESFET Amplifier with Microstrip Components==
 
== Building a Distributed MESFET Amplifier with Microstrip Components==

Revision as of 14:11, 5 September 2015

Tutorial Project: Analyzing Distributed RF Amplifiers With Imported BJT & FET Models
RF150.png

Objective: In this project, the basic concepts of RF.Spice A/D are demonstrated, and a simple voltage divider is modeled and examined.

Concepts/Features:

Minimum Version Required: All versions

'Download2x.png Download Link: [1]

Analyzing Distributed RF Amplifiers With Imported BJT & FET Models

Objective

In the first part of this tutorial, you will learn how to import RF BJT and FET models from text files. In the second part, you will build a distributed RF amplifier using a bilateral RF BJT and generic transmission line components. In the third part, you will build a distributed RF amplifier from an imported unilateral MESFET using physical microstrip components for the input and output matching networks.

Importing High Frequency Transistor Models

RF.Spice's Parts Database contains a sizable collection of RF diodes and BJTs. As you saw in the previous tutorial lesson, each S-Parameter BJT model corresponds to a certain DC operating point. Therefore, you will find a large number of RF BJT models associated with the same device but measured at different values of VCE and IC. The manufacturer data sheets of RF transistors usually contains a table of measured S-parameter data in the following format:


# GHz   s   ma   r   50

freq1     |s11|     ∠s11     |s21|     ∠s21     |s12|     ∠s12     |s22|     ∠s22    

freq2     |s11|     ∠s11     |s21|     ∠s21     |s12|     ∠s12     |s22|     ∠s22    

freq3     |s11|     ∠s11     |s21|     ∠s21     |s12|     ∠s12     |s22|     ∠s22    

...



You can import text files with a ".TXT" file extension containing S-parameter data of the above format to RF.Spice. Better yet, you can create new active RF devices and add them to expand your Parts Database. To create a new device, you need to add the following to lines to the header of your text file:


.model <model_name>

.symbol <symbol_name>


The first line creates a unique model names in the database and the second line picks the right symbol, which is usually either "npn_bjt_2port", or "jfet_n" or "mosfet_n" or "mesfet_n", or their p-type counterparts. For this tutorial lesson, you need to create an RF BJT and an RF MESFET.


The measured data for the RF BJT device are given below:

File Name Model Name Symbol Name Symbol
MyRFBJT.txt MyRFBJT bjt_npn_2port G11A.png
f(GHz) s11 s21 s12 s22
3.0 0.80 ∠ -89 ° 2.86 ∠ 99 ° 0.03 ∠ 56 ° 0.76 ∠ -41 °
4.0 0.72 ∠ -116 ° 2.60 ∠ 76 ° 0.03 ∠ 57 ° 0.73 ∠ -54 °
5.0 0.66 ∠ -142 ° 2.39 ∠ 54 ° 0.03 ∠ 62 ° 0.72 ∠ -68 °


Your MyRFBJT.txt file should look like the following:


.model MyRFBJT

.symbol bjt_npn_2port

3.0 0.80 -89 2.86 99 0.03 56 0.76 -41

4.0 0.72 -116 2.60 76 0.03 57 0.73 -54

5.0 0.66 -142 2.39 54 0.03 62 0.72 -68


The measured data for the MESFET device are given below:

Creating a new active RF device using RF.Spice's Device Editor.


File Name Model Name Symbol Name Symbol
MyMESFET.txt MyMESFET mesfet_n G14A.png
f(GHz) s11 s21 s12 s22
3.0 0.80 ∠ -90 ° 2.80 ∠ 100 ° 0 0.66 ∠ -50 °
4.0 0.75 ∠ -120 ° 2.50 ∠ 80 ° 0 0.60 ∠ -70 °
5.0 0.71 ∠ -140 ° 2.30 ∠ 60 ° 0 0.58 ∠ -85 °


Create two text files as indicated in the tables above. Open RF.Spice's Device Editor and select "Create New RF Device from S-Parameter Test File..." from its RF Menu. Follow the program's prompts step by step and create your new RF BJT and MESFET devices.

Building a Distributed MESFET Amplifier with Microstrip Components

The MESFET Amplifier with microstrip matching networks at its input and output.

The following is a list of parts needed for this part of the tutorial lesson:


AC Voltage Source: VS (keyboard shortcut: Alt+V)

Two 50Ω Resistors: RS and RL

N-Type MESFET: MyMESFET (imported model)

Four Microtrip Line Segments: XMS1, XMS2, XMS3 and XMS4 (keyboard shortcut: Alt+T)

Two Ammeters: AM1 and AM2 (keyboard shortcut: Alt+Y)

Two Net Markers: IN and OUT (keyboard shortcut: Alt+N)



The goal of this part is to design a distributed MESFET amplifier with a gain of 11dB at f = 4GHz. From the S-parameter data of the MESFET, we know that it is a unilateral transistor, i.e. s12 = 0. Moreover, |s11| < 1 and |s22| < 1. Therefore, the MESFET is unconditionally stable. This reduces the input and output reflection coefficients to:

[math] \Gamma_{in} = s_{11} [/math]

[math] \Gamma_{out} = s_{22} [/math]


The conjugate matching conditions at the input and output of the unilateral transistor reduce to:

[math] \Gamma_S = s_{11}^{\ast} [/math]

[math] \Gamma_L = s_{22}^{\ast} [/math]


Furthermore, you have:

[math] G_0 = |s_{21}|^2 = 6.25 = 8.0dB [/math]

[math] G_{Tmax} = G_S . G_0 . G_L = \frac{1}{1- |s_{11}| ^2} . |S_{21}|^2 . \frac{1}{1- |s_{22}| ^2} = 13.5dB [/math]

Using RF.Spice's Device Editor for designing a 50&Omega microstrip line.

To achieve a gain of 11dB, you have 2.5dB more available gain. So you set GS = 2dB and GL = 1dB for a total gain of GT = 2dB + 8dB + 1dB = 11dB. The complex value of ΓS is found on the constant circle GS = 2dB, and the complex value of ΓL is found on the constant circle GL = 1dB, in both cases trying to minimize the distance from the center of the Smith Chart. This requirement yields:

ΓS = 0.33 ∠120°

ΓL = 0.22 ∠70°

The MESFET Amplifier without the source and load sections for the purpose of network analysis.

For your MESFET amplifier, you will use the same input and output matching network types of the previous part consisting of a 50Ω transmission line segment together with a shunt 50Ω Open Stub. For this project, you will use a thin lossless dielectric substrate of thickness h = 0.5mm and relative permittivity &epsilonr = 3.4. A 50Ω microstrip line on this substrate has a width of 1.15mm. At the design frequency of f = 4GHz, the guide wavelength of this microstrip line is λg = 45.74mm.

The lengths of the microstrip segments are found to be:

Microstrip Component Z0 Electrical Length Physical Width Physical Length
XMS1 50Ω 0.179λg 1.15mm 8.19mm
XMS2 50Ω 0.100λg 1.15mm 4.57mm
XMS3 50Ω 0.045λg 1.15mm 2.05mm
XMS4 50Ω 0.432λg 1.15mm 19.76mm

Place and connect all the parts as shown in the above figure. For the shunt stubs, connect the microstrip segments XMS2 and XMS4 in a parallel fashion between the source and load resistors and the ground, respectively. First, remove the AC voltage source and the source and load resistors to perform network analysis. Run a Network Analysis Test of this circuit with start and stop frequencies set at 3GHz and 5GHz, respectively, with a linear frequency step size of 10MHz. Plot the S-parameters on an amplitude-only Cartesian graph. The figure below shows the results for s11, s21, s12 and s22 parameters. Note that since s12 = 0, its dB-scale plot falls at a very large negative number. Therefore, you need to adjust the scale of the vertical axis. The insertion gain |s21| is almost 11dB as expected from the design. However, the value of the return loss |s11| is only -5dB and certainly not very good. This is due to the fact that you had to deliberately introduce a mismatch in the input and output matching networks to achieve the specified gain of 11dB.

The graph of magnitude of s11, s21 and s22 parameters of the MESFET amplifier circuit.

Next, connect the AC voltage source and the source and load resistors and place the source and load ammeters in a similar manner as in the last part of this tutorial lesson. Similarly, define a custom output plot called GP for the power gain of your amplifier. Use the same definition: GP = 20*log10(abs(i(am2)/i(am1))). Run an AC Frequency Sweep Test of your amplifier from 3GHz to 5GHz with linear frequency steps of 10MHz. The figure below shows the graph of power gain vs. frequency.

The graph of the power gain of the MESFET amplifier vs. frequency.

 

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