Dielectric and Conductor-Loss Characterization and Measurements on Electronic Packaging Materials
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
High Q Tunable Filters
High Q Tunable Filters by Fengxi Huang A thesis presented to the University of Waterloo in fulfillment of the thesis requirement for the degree of Doctor of Philosophy in Electrical and Computer Engineering Waterloo, Ontario, Canada, 2012 ©Fengxi Huang 2012 AUTHOR'S DECLARATION I hereby declare that I am the sole author of this thesis. This is a true copy of the thesis, including any required final revisions, as accepted by my examiners. I understand that my thesis may be made electronically available to the public. ii Abstract Microwave tunable filters are key components in radar, satellite, wireless, and various dynamic communication systems. Compared to a traditional filter, a tunable filter is able to dynamically pass the required signal and suppress the interference from adjacent channels. In reconfigurable systems, tunable filters are able to adapt to dynamic frequency selection and spectrum access. They can also adapt to bandwidth variations to maximize data transmission, and can minimize interferences from or to other users. Tunable filters can be also used to reduce size and cost in multi-band receivers replacing filter banks. However, the tunable filter often suffers limited application due to its relatively low Q, noticeable return loss degradation, and bandwidth changing during the filter tuning. The research objectives of this thesis are to investigate the feasibility of designing high Q tunable filters based on dielectric resonators (DR) and coaxial resonators. Various structures and tuning methods that yield relatively high unloaded Q tunable filters are explored and developed. Furthermore, the method of designing high Q tunable filters with a constant bandwidth and less degradation during the tuning process has been also investigated. -
Basic PCB Material Electrical and Thermal Properties for Design Introduction
1 Basic PCB material electrical and thermal properties for design Introduction: In order to design PCBs intelligently it becomes important to understand, among other things, the electrical properties of the board material. This brief paper is an attempt to outline these key properties and offer some descriptions of these parameters. Parameters: The basic ( and almost indispensable) parameters for PCB materials are listed below and further described in the treatment that follows. dk, laminate dielectric constant df, dissipation factor Dielectric loss Conductor loss Thermal effects Frequency performance dk: Use the design dk value which is assumed to be more pertinent to design. Determines such things as impedances and the physical dimensions of microstrip circuits. A reasonable accurate practical formula for the effective dielectric constant derived from the dielectric constant of the material is: -1/2 εeff = [ ( εr +1)/2] + [ ( εr -1)/2][1+ (12.h/W)] Here h = thickness of PCB material W = width of the trace εeff = effective dielectric constant εr = dielectric constant of pcb material df: The dissipation factor (df) is a measure of loss-rate of energy of a mode of oscillation in a dissipative system. It is the reciprocal of quality factor Q, which represents the Signal Processing Group Inc., technical memorandum. Website: http://www.signalpro.biz. Signal Processing Gtroup Inc., designs, develops and manufactures analog and wireless ASICs and modules using state of the art semiconductor, PCB and packaging technologies. For a free no obligation quote on your product please send your requirements to us via email at [email protected] or through the Contact item on the website. -
Agilent Basics of Measuring the Dielectric Properties of Materials
Agilent Basics of Measuring the Dielectric Properties of Materials Application Note Contents Introduction ..............................................................................................3 Dielectric theory .....................................................................................4 Dielectric Constant............................................................................4 Permeability........................................................................................7 Electromagnetic propagation .................................................................8 Dielectric mechanisms ........................................................................10 Orientation (dipolar) polarization ................................................11 Electronic and atomic polarization ..............................................11 Relaxation time ................................................................................12 Debye Relation .................................................................................12 Cole-Cole diagram............................................................................13 Ionic conductivity ............................................................................13 Interfacial or space charge polarization..................................... 14 Measurement Systems .........................................................................15 Network analyzers ..........................................................................15 Impedance analyzers and LCR meters.........................................16 -
Application Note: ESR Losses in Ceramic Capacitors by Richard Fiore, Director of RF Applications Engineering American Technical Ceramics
Application Note: ESR Losses In Ceramic Capacitors by Richard Fiore, Director of RF Applications Engineering American Technical Ceramics AMERICAN TECHNICAL CERAMICS ATC North America ATC Europe ATC Asia [email protected] [email protected] [email protected] www.atceramics.com ATC 001-923 Rev. D; 4/07 ESR LOSSES IN CERAMIC CAPACITORS In the world of RF ceramic chip capacitors, Equivalent Series Resistance (ESR) is often considered to be the single most important parameter in selecting the product to fit the application. ESR, typically expressed in milliohms, is the summation of all losses resulting from dielectric (Rsd) and metal elements (Rsm) of the capacitor, (ESR = Rsd+Rsm). Assessing how these losses affect circuit performance is essential when utilizing ceramic capacitors in virtually all RF designs. Advantage of Low Loss RF Capacitors Ceramics capacitors utilized in MRI imaging coils must exhibit Selecting low loss (ultra low ESR) chip capacitors is an important ultra low loss. These capacitors are used in conjunction with an consideration for virtually all RF circuit designs. Some examples of MRI coil in a tuned circuit configuration. Since the signals being the advantages are listed below for several application types. detected by an MRI scanner are extremely small, the losses of the Extended battery life is possible when using low loss capacitors in coil circuit must be kept very low, usually in the order of a few applications such as source bypassing and drain coupling in the milliohms. Excessive ESR losses will degrade the resolution of the final power amplifier stage of a handheld portable transmitter image unless steps are taken to reduce these losses. -
Tailoring Dielectric Resonator Geometries for Directional Scattering and Huygens’ Metasurfaces
Tailoring dielectric resonator geometries for directional scattering and Huygens’ metasurfaces Salvatore Campione,1,2,* Lorena I. Basilio,2 Larry K. Warne,2 and Michael B. Sinclair2 1Center for Integrated Nanotechnologies (CINT), Sandia National Laboratories, P.O. Box 5800, Albuquerque, NM 87185, USA 2Sandia National Laboratories, P.O. Box 5800, Albuquerque, NM 87185, USA * [email protected] Abstract: In this paper we describe a methodology for tailoring the design of metamaterial dielectric resonators, which represent a promising path toward low-loss metamaterials at optical frequencies. We first describe a procedure to decompose the far field scattered by subwavelength resonators in terms of multipolar field components, providing explicit expressions for the multipolar far fields. We apply this formulation to confirm that an isolated high-permittivity dielectric cube resonator possesses frequency separated electric and magnetic dipole resonances, as well as a magnetic quadrupole resonance in close proximity to the electric dipole resonance. We then introduce multiple dielectric gaps to the resonator geometry in a manner suggested by perturbation theory, and demonstrate the ability to overlap the electric and magnetic dipole resonances, thereby enabling directional scattering by satisfying the first Kerker condition. We further demonstrate the ability to push the quadrupole resonance away from the degenerate dipole resonances to achieve local behavior. These properties are confirmed through the multipolar expansion and show that the use of geometries suggested by perturbation theory is a viable route to achieve purely dipole resonances for metamaterial applications such as wave-front manipulation with Huygens’ metasurfaces. Our results are fully scalable across any frequency bands where high-permittivity dielectric materials are available, including microwave, THz, and infrared frequencies. -
Dielectric Resonator Oscillator Design and Realization at 4.25 Ghz
ELECO 2011 7th International Conference on Electrical and Electronics Engineering, 1-4 December, Bursa, TURKEY Dielectric Resonator Oscillator Design and Realization at 4.25 GHz Şebnem SEÇKİN UĞURLU Department of Electrical and Electronics Engineering Dokuz Eylül University, Izmir, TURKEY [email protected] Abstract device in our circuit. The negative resistance oscillator model is chosen for the design. In the following sections, the design In this paper design and realization of dielectric resonator procedure of the DRO will be considered. oscillator operating 4.25 GHz is explained. The oscillator is designed as a negative resistance oscillator where chip- 2.1 DRO Simulation amplifier is used as the negative resistance by adding feedback. The dielectric resonator is simulated using High The placement of the resonator is an important parameter. Frequency Structure Simulator. The simulation and The width and the length of the microstrip line, as well as the realization results are discussed. distance of the resonator to the microstrip line must be thoroughly analyzed. The resonator is modeled as parallel RLC 1. Introduction resonant circuit and RLC parameters as well as quality factors are calculated from the simulated S-parameter values. It was first presented by R.D. Richtymer [1] that cylindrical For the microstrip substrate, Taconic TLY 3 CH is used. The dielectric structure would act like a resonator. Many years after substrate has a relative dielectric constant of the 2.33 ±.02 and that discovery, such circuits containing dielectric resonators are substrate height of 0.76 mm. As the dielectric resonator, Trans- realized. Tech 8300 series dielectric resonator is used. -
Dielectric Loss
Dielectric Loss - εr is static dielectric constant (result of polarization under dc conditions). Under ac conditions, the dielectric constant is different from the above as energy losses have to be taken into account. - Thermal agitation tries to randomize the dipole orientations. Hence dipole moments cannot react instantaneously to changes in the applied field Æ losses. - The absorption of electrical energy by a dielectric material that is subjected to an alternating electric field is termed dielectric loss. - In general, the dielectric constant εr is a complex number given by where, εr’ is the real part and εr’’ is the imaginary part. Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - Consider parallel plate capacitor with lossy dielectric - Impedance of the circuit - Thus, admittance (Y=1/Z) given by Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - The admittance can be written in the form The admittance of the dielectric medium is equivalent to a parallel combination of - Note: compared to parallel an ideal lossless capacitor C’ with a resistance formula. relative permittivity εr’ and a resistance of 1/Gp or conductance Gp. Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - Input power: - Real part εr’ represents the relative permittivity (static dielectric contribution) in capacitance calculation; imaginary part εr’’ represents the energy loss in dielectric medium. - Loss tangent: defined as represents how lossy the material is for ac signals. Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss The dielectric loss per unit volume: Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - Note that the power loss is a function of ω, E and tanδ. -
Geometry Perturbation of Dielectric Resonator for Same Frequency Operation As Radiator and Filter
32nd URSI GASS, Montreal, 19–26 August 2017 Geometry Perturbation of Dielectric Resonator for Same Frequency Operation as Radiator and Filter Taomia T. Pramiti*(1), Mohamed A. Moharram(1), and Ahmed A. Kishk(1) (1) Electrical and Computer Engineering Department, Concordia University, Montréal, Québec, Canada Abstract using the TM01d mode that provide omnidirectional radia- tion pattern at 2.45GHz. However, having the DR sits on A single dielectric resonator is used for a dual functional a ground plane suppress the TE01d mode. Therefore, it application using the geometry perturbation method at the has to be lifted up using the dielectric substrate. On the desired frequency. The high Q TE01d mode for a filter oper- other hand the resonance frequency of TE01d mode and ation and the low Q TM01d mode for radiation at the same TM01d mode are different. Therefore, geometry perturba- frequency. To operate both modes at the same frequency tion is used to tune the resonance frequency of both modes a circular metallic disk is used to control the energy con- to operate within their bandwidths. In addition, a metallic centrations of the modes inside the dielectric resonator. In disk is placed on the top of the resonator to provide par- addition,a metal disk is used to provide partial shielding for tial shielding for the TE01d mode to enhance its Q-factor. the TE01d mode and allow the TM01d mode radiation and In the design, the metallic disc is also used to improve the at the same time enhance the insertion loss and matching. filter insertion loss without significant effect on the radiat- The design is made for Wi-Fi applications at 2.45 GHz. -
High Dielectric Permittivity Materials in the Development of Resonators Suitable for Metamaterial and Passive Filter Devices at Microwave Frequencies
ADVERTIMENT. Lʼaccés als continguts dʼaquesta tesi queda condicionat a lʼacceptació de les condicions dʼús establertes per la següent llicència Creative Commons: http://cat.creativecommons.org/?page_id=184 ADVERTENCIA. El acceso a los contenidos de esta tesis queda condicionado a la aceptación de las condiciones de uso establecidas por la siguiente licencia Creative Commons: http://es.creativecommons.org/blog/licencias/ WARNING. The access to the contents of this doctoral thesis it is limited to the acceptance of the use conditions set by the following Creative Commons license: https://creativecommons.org/licenses/?lang=en High dielectric permittivity materials in the development of resonators suitable for metamaterial and passive filter devices at microwave frequencies Ph.D. Thesis written by Bahareh Moradi Under the supervision of Dr. Juan Jose Garcia Garcia Bellaterra (Cerdanyola del Vallès), February 2016 Abstract Metamaterials (MTMs) represent an exciting emerging research area that promises to bring about important technological and scientific advancement in various areas such as telecommunication, radar, microelectronic, and medical imaging. The amount of research on this MTMs area has grown extremely quickly in this time. MTM structure are able to sustain strong sub-wavelength electromagnetic resonance and thus potentially applicable for component miniaturization. Miniaturization, optimization of device performance through elimination of spurious frequencies, and possibility to control filter bandwidth over wide margins are challenges of present and future communication devices. This thesis is focused on the study of both interesting subject (MTMs and miniaturization) which is new miniaturization strategies for MTMs component. Since, the dielectric resonators (DR) are new type of MTMs distinguished by small dissipative losses as well as convenient conjugation with external structures; they are suitable choice for development process. -
A Comprehensive Guide to Selecting the Right Capacitor for Your Specific Application
CAPACITOR FUNDAMENTALS EBOOK A Comprehensive Guide to Selecting the Right Capacitor for Your Specific Application 2777 Hwy 20 (315) 655-8710 [email protected] Cazenovia, NY 13035 knowlescapacitors.com CAPACITOR FUNDAMENTALS EBOOK TABLE OF CONTENTS Introduction .................................. 2 The Key Principles of Capacitance and How a Basic Capacitor Works .............................. 3 How Capacitors are Most Frequently Used in Electronic Circuits ............................. 6 Factors Affecting Capacitance .................. 9 Defining Dielectric Polarization .................. 11 Dielectric Properties ........................... 15 Characteristics of Ferroelectric Ceramics ......................... 19 Characteristics of Linear Dielectrics .............. 22 Dielectric Classification ......................... 24 Test Parameters and Electrical Properties .......... 27 Industry Test Standards Overview. 32 High Reliability Testing .......................... 34 Visual Standards For Chip Capacitors ............. 37 Chip Attachment and Termination Guidelines ...... 42 Dissipation Factor and Capacitive Reactance ..... 49 Selecting the Right Capacitor for Your Specific Application Needs ............................ 51 1 CAPACITOR FUNDAMENTALS EBOOK INTRODUCTION At Knowles Precision Devices, our expertise in capacitor technology helps developers working on some of the world’s most demanding applications across the medical device, military and aerospace, telecommunications, and automotive industries. Thus, we brought together our top engineers -
Dielectric Resonators
DIELECTRIC RESONATORS MDR24 SERIES – Ultra High Q Temperature Stable Dielectric Resonators - TE Mode INTRODUCTION MDR24 Series is a specially formulated dielectric material that exhibits Ultra High Q at frequencies between 1.5 and 18 GHz with Qf > 300,000 at 10 GHz. Dielectric Constant is 24 with very tight tolerance. It is ideally suited for high frequency applications where extreme low loss and excellent temperature stability is required. MDR24 Series resonators are available in both disk and cylinder type with or with supports to minimize losses. We recommend alumina and forsterite supports to maintain high Qu factor. Material Characteristics Dielectric Constant ------------------------------------------------------------------------- 24 ± 1 (+/-0.5 Special) o Temperature Coefficient of Resonant Frequency ( τƒ) (ppm/ C) ---------------- 1 to 3 ± 1 Qf (1/tan δ x frequency in GHz) ---------------------------------------------------------- >300,000 @ 10 GHz Thermal Expansion (ppm/ oC) (20 oC) ---------------------------------------------------- >10 Thermal Conductivity (cal/cm-sec oC) @ 25 oC ---------------------------------------- ~ 0.006 Specific Heat (Cal/g oC) -------------------------------------------------------------------- 0.07 Density (g/cc) -------------------------------------------------------------------------------- 7.5 Composition --------------------------------------------------------------------------------- Tantalum Based Color ------------------------------------------------------------------------------------------- -
High Performance Microwave Integrated Filters for 5G Applications
High Performance Microwave Integrated Filters for 5G Applications by Jiacheng Zhang A thesis submitted to the Faculty of Graduate and Postdoctoral Affairs in partial fulfillment of the requirements for the degree of Master of Applied Science in Electrical and Computer Engineering Carleton University Ottawa, Ontario © 2019 Jiacheng Zhang Abstract A 71-76GHz millimeter-wave filter is designed and implemented in a multilayer LTCC module to help attenuate the side spur signal level. The filter is aimed to be embedded in a novel E-band architecture designed at Huawei for millimeter-wave signal communication application. The goal of the filter is to help reduce the third harmonic and fourth harmonic leakage of the LO signal from tripler into the RF channel. Through measurement, for -15dBm received signal power, the 3rd and 4th harmonic leakage levels sof the LO signal is around -25dBc, and both of their frequency range are very close to the transmission band. The designed bandpass filter attenuates the 3rd and 4th harmonic signal power down to -50dBc with a low filter order and small physical size. Unfortunately, access to the fabricated filter was not possible due to existing political tension between the US government and Huawei. The fabricated filter was not shipped to Ottawa, and as a result, it was not measured. A second bandpass filter operating at 10GHz is fabricated using Rogers4360 substrate for measurement and validation. The measurement results show some deviations with simulation results. The center frequency shifts from 10GHz to 11.25GHz. Through analysis, the milling depth of the fabrication process affects the measurement result.