RF MODULE

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NAME EXPRESSION DESCRIPTION b2y 2*pi*a1x/(a1x*a2y-a1y*a2x) y-component of 2nd reciprocal lattice vector n_Air 1 Refractive index of air n_GaAs 3.3285e5[1/m]*lambda0_rfwe+ 3.5031 GEOMETRY MODELING 1 From the Draw menu, choose Specify Objects>Rectangle. 2 In the dialog box that appears, define the rectangle properties according to the table below. WIDTH HEIGHT BASE (X, Y) 3.75e-7 3.75e-7 Center (0, 0) 3 From the Draw menu, choose Specify Objects>Circle. 4 In the dialog box that appears, define the circle properties according to the table below. RADIUS BASE (X, Y) 7e-8 Center (0, 0) 5 Finally, click the Zoom Extents button on the Main toolbar to simplify the boundary and subdomain selection. PHYSICS SETTINGS Boundary Conditions 1 Open the Boundary Settings dialog box from the Physics menu. 2 Select all boundaries and select the Periodic condition from the Boundary condition list. 3 From the Type of periodicity list, choose Floquet periodicity. 4 Enter kx and ky in the edit fields for the k-vector. 5 The selected boundaries represents two groups of periodic conditions, one between Boundaries 1 and 4, and the other between Boundaries 2 and 3. You must specify a different periodic pair index to separate them. Select Boundaries 2 and 3 and enter 2 in the Periodic pair index edit field. 6 Click OK. 246 | CHAPTER 4: OPTICS AND PHOTONICS MODELS Dispersive refractive index of GaAs
Subdomain Settings 1 Open the Subdomain Settings dialog box from the Physics menu and specify the subdomain settings according to the following table. Prior to specifying the refractive index, n, it is necessary to click the Specify material properties in terms of refractive index option button. PROPERTY SUBDOMAIN 1 SUBDOMAIN 2 n n_Air n_GaAs 2 Click the Init tab and enter Ez in the Ez(t 0 ) edit field for both subdomains. 3 Click OK. Integration Coupling Variables When the nonlinear solver calculates the eigenvalue it is necessary to provide a second equation to the system. This model uses a normalization taking the average value of the squared magnitude of the electric field over the entire domain. The average value is calculated using an integration coupling variable, and an ODE forces that variable equal to 1. 1 From the Options menu choose Integration Coupling Variables>Subdomain Variables. 2 In the dialog box that appears, define two variables according to the table below. Make sure that the Global destination check box is selected for both variables. NAME SUBDOMAIN EXPRESSION A 1,2 1 nEz 1,2 Ez*conj(Ez)/A 3 Click OK. BANDGAP ANALYSIS OF A PHOTONIC CRYSTAL | 247
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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
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2 Tutorial Models This chapter cont
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Results and Discussion Figure 2-1 s
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4 Draw a square with corners at (
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COMPUTING THE SOLUTION Click the So
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Results and Discussion The dipole a
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PHYSICS SETTINGS Variables 1 Choose
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5 Click OK to close the dialog box
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Model Library path: RF_Module/Tutor
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4 From the Solve menu, open the Sol
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them from the eigenvalues. The appl
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5 On the Port page, set the values
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5 On the Port page, enter 36.4 in t
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Waveguide Optimization Introduction
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Results and Discussion Figure 2-3 s
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Modeling Using the Graphical User I
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3 Select Boundary 7 and set the Con
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POSTPROCESSING AND VISUALIZATION Fo
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The solution takes a few minutes to
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Night side Earth surface Ionosphere
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Results and Discussion The model pr
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4 Select both spheres and click the
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RF and Microwave Models In this cha
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measure of the transmittance and re
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y 1 cm is at about 7.5 GHz. At the
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By feeding the circulator at a diff
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Importing the Geometry from a Binar
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MESH GENERATION This model uses the
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It is more instructive to look at t
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Note: When displaying S-Parameter v
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Monoconical RF Antenna Introduction
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50 Ω, to obtain maximum transmiss
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Figure 3-7 shows the antenna radiat
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2 Select the RF Module>Electromagne
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13 Zoom in around (0, 0) using the
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4 In the Contour levels area, click
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2 Clear the Keep current plot check
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6 Click the Solve button on the Mai
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Results and Discussion The figure b
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PHYSICS SETTINGS Point Settings Def
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2 In the x-axis area, select the Ex
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Because the impedance is inversely
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4 From the Space dimension list, se
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2 Select Boundaries 1, 2, 4, and 6.
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4 On the Pointwise Constraints page
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12 Click the Solve button on the Ma
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Module. The electromagnetic cavity
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EIGENFREQUENCY VS. TEMPERATURE By r
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GEOMETRY MODELING 1 Go to the Draw
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3 Set dx, dy, and dz to u, v, and w
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20 Select the Solve using solver se
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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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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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3 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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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
Page 203 and 204: inputs are feeding the antenna, lik
Page 205 and 206: the width of the PML is equal to λ
Page 207 and 208: a toggle button that shifts between
Page 209 and 210: 5 Select Coarse solver from the tre
Page 211 and 212: maxE = max(EdB); minE = min(EdB); E
Page 213 and 214: exterior of the PML that shows a ve
Page 215 and 216: 13 Choose Extrude from the Draw men
Page 217 and 218: 2 Click the Settings button. 3 In t
Page 219 and 220: Sea Bed Logging Introduction The Se
Page 221 and 222: Figure 3-39: Electric field magnitu
Page 223 and 224: PHYSICS SETTINGS Scalar Variables 1
Page 225 and 226: 4 Click OK to generate the plot bel
Page 227 and 228: 5 Click the General tab. From the P
Page 229 and 230: Optics and Photonics Models In this
Page 231 and 232: Model Definition The model is built
Page 233 and 234: Model Library path: RF_Module/Optic
Page 235 and 236: PHYSICS SETTINGS Scalar Variables S
Page 237 and 238: POSTPROCESSING AND VISUALIZATION By
Page 239 and 240: Model Definition The geometry is a
Page 241 and 242: 2 In the list of application modes,
Page 243 and 244: Because the refractive index of GaA
Page 245 and 246: 5 Click OK twice to see the followi
Page 247 and 248: Bandgap Analysis of a Photonic Crys
Page 249 and 250: a 2 a 3 × b1 = 2π----------------
Page 251 and 252: The five lowest bands for the (1, 1
Page 253: Modeling Using the Graphical User I
Page 257 and 258: 3 Click the Parametric tab. Select
Page 259 and 260: 3 Click OK to see the following plo
Page 261 and 262: fem.appl{1}.prop.analysis = 'harmon
Page 263 and 264: Model Definition The mode analysis
Page 265 and 266: 2 Select the RF Module>Perpendicula
Page 267 and 268: 4 On the Contour page, give Magneti
Page 269 and 270: includes only two independent param
Page 271 and 272: OPTIONS AND SETTINGS 1 Open the Con
Page 273 and 274: The problem becomes well-posed by a
Page 275 and 276: POSTPROCESSING AND VISUALIZATION Th
Page 277 and 278: 7 Click OK. 8 From the Postprocessi
Page 279 and 280: the computed propagation constants
Page 281 and 282: 3 The default eigenmode is the one
Page 283 and 284: Compare these ideal values of the p
Page 285 and 286: Stress-Optical Effects with General
Page 287 and 288: The PDE solved is Navier’s equati
Page 289 and 290: and εx ∂u = ∂x εy ∂v = ∂y
Page 291 and 292: Model Library path: RF_Module/Optic
Page 293 and 294: NAME EXPRESSION DESCRIPTION B2 0.65
Page 295 and 296: 2 In the Subdomain Expressions dial
Page 297 and 298: 4 Initialize the mesh in this geome
Page 299 and 300: Note: This model includes an extens
Page 301 and 302: 3 Enter 1.46 in the text field Sear
Page 303 and 304: 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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