RF MODULE

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SCALAR VARIABLES 1 From the Physics menu, select Scalar Variables. 2 In the Application Scalar Variables dialog box, set the Frequency to freq. 3 Click OK. PHYSICS SETTINGS Boundary Conditions The default boundary condition is perfect electric conductor which is fine for all exterior boundaries except at the ports. Interior boundaries are by default not active meaning that continuity is imposed. 1 From the Physics menu, choose Boundary Settings. 2 At Boundaries 1, 20, and 21, specify the Port boundary condition. On the Conditions and Port pages set the values according to the following table; when done, click OK. SETTINGS BOUNDARY 1 BOUNDARY 20 BOUNDARY 21 Port number 1 3 2 Wave excitation at this port Selected Cleared Cleared Mode specification Analytic Analytic Analytic Mode number 1 1 1 Subdomain Settings 1 From the Physics menu, choose Subdomain Settings. 2 In the Subdomain Settings dialog box, click the Groups tab and create three groups called air, dielectric, and ferrite, respectively, by clicking the New button and replacing new group in the Name edit field with the name of each group. 3 Keep the default subdomain settings for the air group. For the dielectric group, change the Relative permittivity to eps_r. For the ferrite group, set the Relative permittivity to 12.9, and enter the Relative permeability, as four space-separated entries in this edit field: mur -i*kr i*kr mur. 4 On the Subdomains page, assign Subdomains 1, 3, 6, and 7 to the air group; Subdomains 2, 4, and 5 to the dielectric group; and Subdomain 8 to the ferrite group. 5 Click OK. 58 | CHAPTER 3: <strong>RF</strong> AND MICROWAVE MODELS
MESH GENERATION This model uses the default mesh as initial mesh for the adaptive meshing. It is important to remember to initialize the mesh prior to each new solution step. Otherwise the solver applies the adaptive mesh refinement algorithm on an already adapted mesh. COMPUTING THE SOLUTION Use the parametric solver to study the S-parameters as a function of the relative permittivity in the matching elements. Also activate adaptive meshing on the S11-parameter. 1 Click the Solver Parameters button on the Main toolbar. 2 From the Solver list, select Parametric. 3 Enter eps_r as Parameter names and range(1,0.01,1.5) as Parameter values. The solver will calculate the solution for 51 equidistant permittivity values in the range 1 to 1.5. 4 Select the Adaptive mesh refinement check box. 5 Go to the Adaptive page. From the Error estimate list, choose Functional. Then type S11_rfwe in the Functional edit field. 6 Click OK. 7 Click the Solve button on the Main toolbar. The solver performs a full sweep before each adaptive mesh refinement. It is possible to speed up the parameter sweep by first doing the adaptive meshing for one parameter value, and then turn off the adaptive mesh refinement before running the full sweep. THREE-PORT FERRITE CIRCULATOR | 59
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COMSOL Multiphysics RF MODULE V ERS
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CONTENTS Chapter 1: Introduction Mo
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Results and Discussion. . . . . . .
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Chapter 4: Optics and Photonics Mod
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1 Introduction The RF Module Model
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highlights. The categories here inc
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TABLE 1-1: RF MODULE MODEL LIBRARY
Page 15 and 16: 2 Tutorial Models This chapter cont
Page 17 and 18: Results and Discussion Figure 2-1 s
Page 19 and 20: 4 Draw a square with corners at (
Page 21 and 22: COMPUTING THE SOLUTION Click the So
Page 23 and 24: Results and Discussion The dipole a
Page 25 and 26: PHYSICS SETTINGS Variables 1 Choose
Page 27 and 28: 5 Click OK to close the dialog box
Page 29 and 30: Model Library path: RF_Module/Tutor
Page 31 and 32: 4 From the Solve menu, open the Sol
Page 33 and 34: them from the eigenvalues. The appl
Page 35 and 36: 5 On the Port page, set the values
Page 37 and 38: 5 On the Port page, enter 36.4 in t
Page 39 and 40: Waveguide Optimization Introduction
Page 41 and 42: Results and Discussion Figure 2-3 s
Page 43 and 44: Modeling Using the Graphical User I
Page 45 and 46: 3 Select Boundary 7 and set the Con
Page 47 and 48: POSTPROCESSING AND VISUALIZATION Fo
Page 49 and 50: The solution takes a few minutes to
Page 51 and 52: Night side Earth surface Ionosphere
Page 53 and 54: Results and Discussion The model pr
Page 55 and 56: 4 Select both spheres and click the
Page 57 and 58: RF and Microwave Models In this cha
Page 59 and 60: measure of the transmittance and re
Page 61 and 62: y 1 cm is at about 7.5 GHz. At the
Page 63 and 64: By feeding the circulator at a diff
Page 65: Importing the Geometry from a Binar
Page 69 and 70: It is more instructive to look at t
Page 71 and 72: Note: When displaying S-Parameter v
Page 73 and 74: Monoconical RF Antenna Introduction
Page 75 and 76: 50 Ω, to obtain maximum transmiss
Page 77 and 78: Figure 3-7 shows the antenna radiat
Page 79 and 80: 2 Select the RF Module>Electromagne
Page 81 and 82: 13 Zoom in around (0, 0) using the
Page 83 and 84: 4 In the Contour levels area, click
Page 85 and 86: 2 Clear the Keep current plot check
Page 87 and 88: 6 Click the Solve button on the Mai
Page 89 and 90: Results and Discussion The figure b
Page 91 and 92: PHYSICS SETTINGS Point Settings Def
Page 93 and 94: 2 In the x-axis area, select the Ex
Page 95 and 96: Because the impedance is inversely
Page 97 and 98: 4 From the Space dimension list, se
Page 99 and 100: 2 Select Boundaries 1, 2, 4, and 6.
Page 101 and 102: 4 On the Pointwise Constraints page
Page 103 and 104: 12 Click the Solve button on the Ma
Page 105 and 106: Module. The electromagnetic cavity
Page 107 and 108: EIGENFREQUENCY VS. TEMPERATURE By r
Page 109 and 110: GEOMETRY MODELING 1 Go to the Draw
Page 111 and 112: 3 Set dx, dy, and dz to u, v, and w
Page 113 and 114: 20 Select the Solve using solver se
Page 115 and 116: Computing the Solution Using a Para
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8 Click Solve. 9 When the parametri
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H-Bend Waveguide with S-parameters
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Model Library path: RF_Module/RF_an
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1 From the Postprocessing menu, cho
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The rectangular port is excited by
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Figure 3-16 shows a single-mode wav
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Figure 3-18: The S 21 parameter (in
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PHYSICS SETTINGS First set up the b
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FREEZING THE BOUNDARY MODE ANALYSIS
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12 Click the Solve button on the Ma
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Microwave Cancer Therapy Introducti
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The model takes advantage of the pr
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DOMAIN AND BOUNDARY EQUATIONS—HEA
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Figure 3-23: The computed microwave
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solutions for both the electromagne
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4 Select Subdomain 1, then enter th
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1 Click the Plot Parameters button
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sar_in_human_head_interp.txt. That
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The bioheat equation produces a sim
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3 Click OK. 4 From the Options menu
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17 In the Work-Plane Settings dialo
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SETTINGS SUBDOMAIN 19 epsilonr_brai
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4 Click the Init tab and type 0 in
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POSTPROCESSING AND VISUALIZATION 1
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The walls of the oven and the waveg
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Figure 3-29: Temperature in the cen
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3 Click the block symbol again and
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2 At the waveguide end, Boundary 23
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4 Click OK to generate the plot bel
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Because the filter cutoff should be
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the force is applied. Figure 3-32 d
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6 Then the ECAD Import Options dial
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PHYSICS SETTINGS Subdomain Settings
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solver takes more steps than it sto
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3 Select Subdomain 1 and clear the
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13 Click the Solve button on the Ma
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Balanced Patch Antenna for 6 GHz In
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k0 = ω ε0 µ 0 All metallic objec
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divided by the input power. In Figu
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Reference 1. E. Recht and S. Shiran
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10 Select the objects SQ2, CO1, and
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43 Specify two spheres with the fol
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inputs are feeding the antenna, lik
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the width of the PML is equal to λ
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a toggle button that shifts between
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5 Select Coarse solver from the tre
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maxE = max(EdB); minE = min(EdB); E
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exterior of the PML that shows a ve
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13 Choose Extrude from the Draw men
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2 Click the Settings button. 3 In t
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Sea Bed Logging Introduction The Se
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Figure 3-39: Electric field magnitu
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PHYSICS SETTINGS Scalar Variables 1
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5 Click the General tab. From the P
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Optics and Photonics Models In this
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Model Definition The model is built
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Model Library path: RF_Module/Optic
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PHYSICS SETTINGS Scalar Variables S
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POSTPROCESSING AND VISUALIZATION By
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Model Definition The geometry is a
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2 In the list of application modes,
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Because the refractive index of GaA
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5 Click OK twice to see the followi
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Bandgap Analysis of a Photonic Crys
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a 2 a 3 × b1 = 2π----------------
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The five lowest bands for the (1, 1
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Modeling Using the Graphical User I
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Subdomain Settings 1 Open the Subdo
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3 Click the Parametric tab. Select
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3 Click OK to see the following plo
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fem.appl{1}.prop.analysis = 'harmon
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Model Definition The mode analysis
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2 Select the RF Module>Perpendicula
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4 On the Contour page, give Magneti
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includes only two independent param
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OPTIONS AND SETTINGS 1 Open the Con
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The problem becomes well-posed by a
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POSTPROCESSING AND VISUALIZATION Th
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7 Click OK. 8 From the Postprocessi
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the computed propagation constants
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3 The default eigenmode is the one
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Compare these ideal values of the p
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Stress-Optical Effects with General
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The PDE solved is Navier’s equati
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and εx ∂u = ∂x εy ∂v = ∂y
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Model Library path: RF_Module/Optic
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NAME EXPRESSION DESCRIPTION B2 0.65
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2 In the Subdomain Expressions dial
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4 Initialize the mesh in this geome
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Note: This model includes an extens
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3 Enter 1.46 in the text field Sear
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In these expressions, w 0 is the mi
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After 90 fs the pulse has reached t
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4 Select the RF Module>In-Plane Wav
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Boundary Conditions 1 From the Phys
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6 Click the Remesh button; when the
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2 On the General page, make sure th
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Propagation of a 3D Gaussian Beam L
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Figure 4-15: After 20 fs the pulse
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7 Click the Delete Interior Boundar
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Boundary Conditions 1 From the Phys
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5 From the Options menu, select Sup
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INDEX 3D electromagnetic waves mode
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efractive index 222, 254 resistance
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RF MODULE

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