International Journal of Engineering Trends and Technology (IJETT) – Volume 14 Number 4 – Aug 2014 Characterization of Circular Waveguide at High Frequency Kalpesh K. Prajapati#1, Prof. Rajesh Ishwar#2 #1 .P.G. Student, Department of Electronics and Communication S.P.B. Patel Engineering College, Linch , Mehsana, India #2 .Assi. professor, Department of Electronics and Communication S.P.B.Patel Engineering College, Linch , Mehsana, India Abstract : In the recent years there is a notable development leap in communication system operating at Microwave frequencies. Such a development is necessary to support a wide variety of emerging application. In this paper the characterization of Circular waveguide is done at high frequency of 20 Ghz. The characteristics like E-field , H-field, VSWR , S-parameter is observed. The Simulation is carried out in the HFSS (High Frequency Simulation Software). keyword: Circular waveguide, VSWR, Propagation Constant, HFSS I. INTRODUCTION The circular waveguide is a transmission line which is in the circular shape. The characterization of the circular waveguide is done by transmitting wave from hollow waveguide with a air or vacuum filled material. The reflection of the wave from the wall and travelling through the circular waveguide will demonstrate the characteristics of the component. Circular waveguide is the passive microwave component. The passive Component are those component which does not required any external power supply for its operation. The electromagnetic waves propagating inside the waveguide may be characterized by reflections from the conducting walls. It is a radiating structure finds many applications in communication system, radar, biomedical, and both as single radiator and as coupled radiators. The Circular waveguide is a transmission medium supports TE and TM modes. Because of the lack of a center conductor, the electromagnetic field supported by a waveguide can only be TE or TM modes. For circular waveguide the dominant mode is TE11, which has the lowest cut-off frequency. The HFSS is a software package analysis modeling and analysis of 3-dimensional structures. HFSS utilizes a 3D full wave finite element method to compute the electrical behaviors of high frequency and high speed components. The HFSS is more accurately characterizes the electrical performance of components and effectively evaluates various parameters. It helps the user to observe and ISSN: 2231-5381 analyze various performance of electromagnetic properties of structures such as propagation constant, characteristic port impedance, generalized S-parameters and YParameter etc are normalized to specific port impedances, the Eigen modes or resonances of the of the structures. The HFSS software is designed for extracting modal parameters by simulating passive devices. It is necessary for designing high frequency and high speed components used in modern electronic devices. The HFSS simulated results are more accurate and helpful before design and fabricating of real world components. In this paper characteristic of the Circular waveguide is simulated using HFSS. This analysis is much helps in the fundamental of waveguide. II. METHODOLOGY Electromagnetic field can be predicted by experiment, analysis and computation. The last mentioned technique, otherwise known as numerical simulation, is the most recent and rapidly advancing. Electromagnetic field, like many other physical processes, are governed by partial deferential equations (PDEs). Hence the numerical methods for solving such problems can be classed with other methods of solving PDEs, such as the Finite Element method, Method of Moments and Finite Deference method. Every modeling technique has some strengths and some weaknesses. Electromagnetic simulators can give very accurate solutions for microwave circuits with ideal conductors. When the conductors are non-ideal, accurate results may still be obtained in many cases by specifying material parameters or surface impedances. However, for structures in which the penetration depth of the field into the conductors is of the same order as the conductor thickness, considerable error can occur. The finite element method is one of the most successful frequency domain computational methods for electromagnetic simulations. The method’s main advantage is its capability to treat any type of geometry and material in homogeneity without a need to alter the http://www.ijettjournal.org Page 158 International Journal of Engineering Trends and Technology (IJETT) – Volume 14 Number 4 – Aug 2014 III. SIMULATION formulation or the computer code. That is, it provides geometrical fidelity and unrestricted material treatment. A circular waveguide is a tubular , circular conductor. A plane wave propagating through a circular waveguide results in transverse electric (TE) or transverse magnetic (TM) mode. The design of the circular waveguide is created in the HFSS simulation software. The driven model solution is selected for the simulation. the design in the HFSS is as below in Fig. 2. The waveguide is filled with the vacuum and assigned boundary condition is finite conductivity. The excitation is provided at both the wave port. Fig. 1 Coordinates of a Circular waveguide It is commonly assumed that the waves in a circular waveguide are propagating in the positive z direction. The modes in the circular guide are characterized by = 0.This means that the z component of the magnetic field must exist in the guide in order to have electromagnetic energy transmission. A Helmholtz equation for in a circular guide is given by ∇ = (1) Fig.2 Circular waveguide in HFSS The Design of circular waveguide with the inner diameter of 2.383 cm (0.938 in.) in HFSS. The outer wall of the waveguide is assigned a boundary condition called finite conductivity or perfect E. with this assumption, the port is defined within a waveguide. The frequency range for the simulation is 0-20 GHZ. IV. RESULT Its solution is given by ( = )cos( ∅) The output for the different modes of the port are seen in the simulation result. The result for the , for the mode 1 and for the for mode 2 are seen in the simulation , analysis. (2) Which is subject to boundary condition. . The modes in the circular guide are characterized by = 0.However, the z component of the electric field must exist in order to have energy transmission in guide. Consequently, the Helmholtz equation for in a circular guide is given by ∇ = (3) Its solution is given by = ( )cos( ∅) Fig.3 (4) , mode 1. Which is subject to boundary condition. ISSN: 2231-5381 http://www.ijettjournal.org Page 159 International Journal of Engineering Trends and Technology (IJETT) – Volume 14 Number 4 – Aug 2014 Fig.3 , Mode 2 Fig.6 H field Pattern The output of the VSWR plot for the circular waveguide indicates the reflection of travelling wave in the waveguide. The standing wave ratio for the circular waveguide from the simulation is as below. VSWR HFSSDesign1 1.0035 ANSOFT Curve Info VSWR(w aveport1:1) Setup1 : Sw eep VSWR(w aveport2:2) Setup1 : Sw eep 1.0030 1.0025 V. CONCLUSION The characterization of the circular waveguide in the high frequency is done in the simulation software HFSS. The output results for the different modes , VSWR and field shows that waveguide is working perfectly at this frequency. The waveguide is ready to work in the open environment for its different application. ACKNOWLEGMENT Y1 1.0020 1.0015 1.0010 1.0005 1.0000 0.00 2.50 5.00 7.50 10.00 Freq [GHz] 12.50 15.00 17.50 20.00 To present this paper I would like to thanks Prof. J.C. Prajapati for his continues motivation and guidance. I would also like to thanks the Laboratory assistants of Saffrony College for help in using the lab component very effectively. REFRENCES Fig.4 VSWR plot The field pattern for the travelling E-filed and H-filed wave in the waveguide. Fig.5 E Field Pattern ISSN: 2231-5381 [1] Channbasyya Methad , Paramesha , D Srinivasa Rao,"Characterization of rectangular waveguide using HFSS."IJEEDC ISSN (PRINT): 2320-2084, Volume–1, Issue – 1, 2013 [2] Pampa Debnath , Snehasis Roy, "An analysis of waveguide magic tee at x band using HFSS." Volume 2, Issue 5, May 2012. [3] S.Paramesha and A, Chakrabarty “Waveguide as a near- field measuring probe of the two element array radiator” Progress in Electromagnetics Reasearch PIER B, vol. 7, 245-255, 2008. [4] Jiao, C. 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