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Doruk Senkal - Whole-angle MEMs gyroscopes: challenges and opportunities

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Whole-angle MEMs gyroscopes: challenges and opportunities: summary, description and annotation

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Coriolis Vibratory Gyroscopes (CVGs) can be divided into two broad categories based on the gyroscopes mechanical element: (Type 1) degenerate mode gyroscopes, which have x-y symmetry, and (Type 2) non-degenerate mode gyroscopes, which are designed intentionally to be asymmetric in x and y modes. Currently, non-degenerate mode gyroscopes fulfill the needs of a variety of commercial applications, such as tilt detection, activity tracking, and gaming. However, when it comes to inertial navigation, where sensitivity and stability of the sensors are very important, commercially available MEMS sensors fall short by three orders of magnitude. Degenerate mode gyroscopes on the other hand, have a number of unique advantages compared to non-degenerate vibratory rate gyroscopes, including higher rate sensitivity, ability to implement whole-angle mechanization with mechanically unlimited dynamic range, exceptional scale factor stability, and a potential for self-calibration. For this reason, as the MEMS gyroscope development is reaching maturity, the Research and Development focus is shifting from high-volume production of low-cost non-degenerate mode gyroscopes to high performance degenerate mode gyroscopes. This paradigm shift in MEMS gyroscope research and development creates a need for a reference book to serve both as a guide and an entry point to the world of degenerate mode gyroscopes--

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Table of Contents List of Tables List of Abbreviations Chapter 5 Chapter - photo 1
Table of Contents
List of Tables
  1. List of Abbreviations
  2. Chapter 5
  3. Chapter 7
  4. Chapter 8
List of Illustrations
  1. Chapter 1
  2. Chapter 2
  3. Chapter 3
  4. Chapter 4
  5. Chapter 5
  6. Chapter 6
  7. Chapter 7
  8. Chapter 8
  9. Chapter 9
Guide
Pages

IEEE Press
445 Hoes Lane
Piscataway, NJ 08854

IEEE Press Editorial Board
Ekram Hossain, Editor in Chief

Jn Atli BenediktssonDavid Alan GrierElya B. Joffe
Xiaoou LiPeter LianAndreas Molisch
Saeid NahavandiJeffrey ReedDiomidis Spinellis
Sarah SpurgeonAhmet Murat Tekalp
Whole-Angle MEMS Gyroscopes
Challenges and Opportunities

Doruk Senkal

Andrei M. Shkel

Copyright 2020 by The Institute of Electrical and Electronics Engineers Inc - photo 2

Copyright 2020 by The Institute of Electrical and Electronics Engineers, Inc. All rights reserved.

Published by John Wiley & Sons, Inc., Hoboken, New Jersey.
Published simultaneously in Canada.

No part of this publication may be reproduced, stored in a retrieval system, or transmitted in any form or by any means, electronic, mechanical, photocopying, recording, scanning, or otherwise, except as permitted under Section 107 or 108 of the 1976 United States Copyright Act, without either the prior written permission of the Publisher, or authorization through payment of the appropriate per-copy fee to the Copyright Clearance Center, Inc., 222 Rosewood Drive, Danvers, MA 01923, (978) 750-8400, fax (978) 750-4470, or on the web at www.copyright.com. Requests to the Publisher for permission should be addressed to the Permissions Department, John Wiley & Sons, Inc., 111 River Street, Hoboken, NJ 07030, (201) 748-6011, fax (201) 748-6008, or online at http://www.wiley.com/go/permission.

Limit of Liability/Disclaimer ofWarranty: While the publisher and author have used their best efforts in preparing this book, they make no representations or warranties with respect to the accuracy or completeness of the contents of this book and specifically disclaim any implied warranties of merchantability or fitness for a particular purpose. No warranty may be created or extended by sales representatives or written sales materials. The advice and strategies contained herein may not be suitable for your situation. You should consult with a professional where appropriate. Neither the publisher nor author shall be liable for any loss of profit or any other commercial damages, including but not limited to special, incidental, consequential, or other damages.

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Wiley also publishes its books in a variety of electronic formats. Some content that appears in print may not be available in electronic formats. For more information aboutWiley products, visit our web site at www.wiley.com.

Library of Congress Cataloging-in-Publication Data is applied for

ISBN 9781119441885

Cover Design: Wiley
Cover Image: Courtesy of Doruk Senkal

List of Abbreviations

Table 1 Control system abbreviations.

SymbolDescription
QuadratureUnwanted component of oscillation that interferes with estimation of the pattern angle, manifests as a result of structural imperfections
AGCAmplitude Gain Control, closedloop control of drive amplitude
PLLPhase Locked Loop, closedloop control system that generates an AC signal with a predetermined phase offset from the resonator
FTRForcetorebalance, closedloop control system that actively drives the pattern angle to a setpoint
Quadrature nullClosedloop control system that actively suppresses the effects of structural imperfections within the gyroscope

Table 2 Mechanical parameters of the resonator.

SymbolDescription
fMean frequency of the two primary modes of the resonator
Mean energy decay time constant of the resonator
QfactorRatio of stored energy to energy loss per vibration cycle (Q = f)
fFrequency split between primary modes in Hz (f = fxfy)
Frequency split between primary modes in rad/s ( = xy)
1Measure of anisodamping within the gyroscope (Whole-angle MEMs gyroscopes challenges and opportunities - image 3)
Angle defining the orientation of actual versus intended axes of elasticity
Angle defining the orientation of actual versus intended axes of damping
(x, y, z)Coordinate frame oriented along intended axes of symmetry x and y
n = 2 modeA 4node degenerate mode pair of a wineglass or ring/disk system
n = 3 modeA 6node degenerate mode pair of a wineglass or ring/disk system
Precession patternVibration pattern formed by superposition of x and y vibratory modes, which is capable of changing its orientation (precesses) when subjected to Coriolis forces or an external forcing function
Pattern angle ()Orientation of the precession pattern in degrees, which is a measure of angular rotation in a Rate Integrating Gyroscope
Preface

Coriolis Vibratory Gyroscopes (CVGs) can be divided into two broad categories based on the gyroscope's mechanical element: degenerate mode gyroscopes (type 1), which have xy symmetry, and nondegenerate mode gyroscopes (type 2), which are designed intentionally to be asymmetric in x and y modes.

Currently, nondegenerate mode gyroscopes fulfill the needs of a variety of commercial applications, such as tilt detection, activity tracking, and gaming. However, when it comes to inertial navigation, where sensitivity and stability of the sensors are very important, commercially available MEMS sensors fall short by three orders of magnitude. Degenerate mode gyroscopes, on the other hand, offer a number of unique advantages compared to nondegenerate vibratory rate gyroscopes, including higher rate sensitivity, ability to implement wholeangle mechanization with mechanically unlimited dynamic range, exceptional scale factor stability, and a potential for selfcalibration. For this reason, as the MEMS gyroscope development is reaching maturity, the Research and Development focus is shifting from highvolume production of lowcost nondegenerate mode gyroscopes to high performance degenerate mode gyroscopes. This paradigm shift in MEMS gyroscope research and development creates a need for a reference book to serve both as a guide and an entry point to the field of degenerate mode gyroscopes.

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