Measure Angular Motion of a Mems-Based Gyroscope

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The graduate students at GIKI have worked on the development of MEMS-based gyroscopes. For this purpose a rate table was required for the MEMS lab in order to test these gyroscopes. Hence this task was undertaken at undergraduate level in the form of a final year project. The purpose of this was to create technical awareness of MEMS technology at an undergraduate level plus achieve the required goal in a very cost effective manner. Problem Definition

The task was to indigenously develop a rate table which not only is cost-effective but also delivers performance parameters. Aim
The aim was to design a single-axis rate table. On the top of the rate table, IC (gyroscope) shall be mounted. From a PC through a controller, the rate table shall be rotated at the required rate (rpm). All the connections to the IC shall be available through the non-rotating base of the table. Time line

Date| Event|
Sep ‘08| * Project proposal * Collection of data * Analysis of Data * Project approval| Oct ‘08| * Understanding of Rate Tables * Initial Design of Rate Table| Nov ‘08| * Simulation results * Status report of Hardware & Software| Jan ‘09| * Design of Controller * Design of Rate Table| Feb ‘09| * Implementation of Hardware design * Integration of Hardware & Software| Mar ‘09| * Testing and Troubleshooting|

Apr ‘09| * Open House * Final Report and Thesis|

* Open House * Final Report and Thesis| * All * All|

Chapter 2
Introduction to Rate Table
Rate table is a device which is widely used for testing and calibrating instruments such as precision gyros and accelerometers which comprise the basic sensors in high-accuracy inertial guidance systems. Because these sensing instruments are capable of measuring extremely minute dynamic quantities, formidable demands are placed on the rate tables used for supplying known inputs to these instruments. Thus, to be compatible with the accuracy of gyros and accelerometers currently in use, a rate table system must be capable of measuring and controlling angular velocities down to the order of 0.001 degree per second. Single-Axis test tables provide precise angular position, rate and acceleration for development and production testing of inertial components and systems. What is Gyroscope?

Micro machined inertial sensors, consisting of accelerometers and gyroscopes are one of the most important types of silicon based sensors. A gyroscope is a device for measuring or maintaining orientation, based on the principles of angular momentum.

The Gyroscope developed at GIKI is a thermally actuated 3-DoF micro-machined gyroscope utilizing Chevron thermal actuators to drive proof mass. There are a number of actuation mechanisms which include electrostatic, piezoelectric, thermal etc. The benefits of this design will be described later.

These actuators are activated by Joule heating. When a potential difference is applied between two or more points on electrically conducting material it causes flow of electrical current which induces thermal strain due to internal heating. Consequently these thermal strains generate the desired mechanical deformation or force. These thermal actuators are capable of providing a large force.

There are two types of thermal actuators: hot/cold arm thermal actuators and ‘V’ or Chevron’ shaped actuators.

The displacement in Chevron actuators is proportional toV2.

Mass m1 is constrained to oscillate only in the drive direction (1-DOF) whereas the mass m2 is free to oscillate in both drive (X-axis) and sense (Y-axis) direction (2-DOF). This makes the system a 3-DOF one. Mass m1 is excited in the drive direction. When the system is rotated a Coriolis force acts on mass m2 which can be measured using capacitance changes. This information in turn can be used to determine the rotation or orientation of the system.

Advantages of this design:

High force, large displacement and low voltage consumption are the primary concerns for micro-gyroscopes. In comb drive actuators, a p.d. of 20V causes a displacement of 5µm whereas in Chevron based thermal actuators a p.d. of only 0.1V causes a displacement of 5.5µm.

Gyroscope Testing:

* In gyroscope testing we stimulate the gyroscope by mounting it on the rate table. * Rate table provides the gyroscope precise angular motion about one or several axis. * This angular motion causes capacitance changes in the gyroscope. * This capacitance change will be used to measure rotation and orientation Commercially available Rate Table

Rate tables are designed to provide precise position, rate and acceleration motion for development or production testing. This test instrument is used for the testing and calibration of sensors and gyroscopic instruments which require a precise and accurate angular velocity. During the study we came across the vendors of the testing equipment. Ideal Aerosmith, EVO-10 and Acutronic are the market leaders.

Comm. Interface| RS232, Ethernet |

Chapter 3
Design
Hardware
The hardware requirement for the fabrication of the rate table is: * Motor
* Gyroscope IC
* DC power supply
* Slip rings
* Controller
* RS 232 Interface
* Lathe Machine
* Shaper Machine
* Personal Computer (PC)
* Micromachining Device

Motor
A brushless DC motor (BLDC) is a synchronous electric motor which is powered by direct-current electricity (DC) and which has an electronically controlled commutation system, instead of a mechanical commutation system based on brushes. In such motors, current and torque, voltage and rpm are linearly related. BLDC motors are considered to be more efficient than brushed DC motors. BLDC motors offer several advantages over brushed DC motors this includes higher efficiency and reliability, reduced noise, longer lifetime (no brush erosion), elimination of ionizing sparks from the commutator, and overall reduction of electromagnetic interference (EMI). Comparison of conventional and brushless DC motors:

The motor used in the Rate Table is a brushless DC motor and driver package with digital operator. It is a product of Oriental Motors. It is the BLF series with the model number BLF 460C-200.

Specifications:
Model BLF460C-□Combination Type – Parallel Shaft Gear head| Rated Output Power (Continuous) W (HP)| 60 (1/12)| Rated voltage V| Single-Phase 200–240 _10%| Rated frequency Hz| 50/60 _5%| Rated input current A| 1.2| Maximum input current A| 3.0| Rated Torque N_ m (oz-in)| 0.2 (28.4)| Starting torque N_ m (oz-in)| 0.4 (56.8)| Rated speed r/min| 3000| Speed control range r/min| 80_4000|

Slip Rings
A slip ring is an electromechanical device that allows the transmission of power and electrical signals from a stationary to a rotating structure. Also called a rotary electrical joint, collector or electric swivel, a slip ring can be used in any electromechanical system that requires un-restrained, intermittent or continuous rotation while transmitting power and/or data. It can improve mechanical performance, simplify system operation and eliminate damage-prone wires dangling from movable joints. The slip ring used in the Rate Table is by MOOG Inc., model no. AC 6355- 36. The specification and the diagram for the slip rings are stated below. Operating Speed| 250 rpm|

Mercotac
Mercotac are mercury-based electrical connectors superior to slip rings. The electrical conduction path is a liquid metal that is molecularly bonded to the contacts. This creates a connection that is constant and unchanged for the life of the connector. Mercotac connectors are maintenance free, do not degrade the signal over time and last much longer than slip rings. They transmit with near zero electrical noise, thus the same connector can be used for power and signal transmission.

Amongst the various models available, the most appropriate one that seemed for the Rate Table was Model 830. Below are the specifications and diagram for the model.

Model No.| Conductors| Description| Voltage AC/DC| Max. Freq. MHz| Contact Resistance| Max OP. RPM| AMP Ratingat 240 VAC| TemperatureMax. F (C) / Min.F (C)| RotationTorque (gm-cm)| 830| 8| Standard Model| 0-250| 100| <1m| 200| 2@4/6@30| 140(60)/-20(-29)| 1000| 830 SS| 8| Stainless Steel Bearing| 0-250| 100| <1m| 200| 2@4/6@30| 140(60)/-20(-29)| 1000|

ACKNOWLEDGEMENTS

Firstly, we are thankful to Allah Almighty for his grace and mercy he bestowed upon us throughout. We thank Him for his blessings and guidance. We would like to express profound gratitude to our advisor, Dr. Shafat. A. Bazaz, for his invaluable support, encouragement, supervision and useful suggestions throughout this project work. His moral support and continuous guidance enabled us to complete our work successfully. We are also highly thankful to Faculty of Electronics Engineering, GIKI, for their valuable suggestions throughout this study. From the staff, Mr. Iftikhar (store keeper) and Mr. Abdullah Jan (PS to dean) are especially thanked for their care and attention. We would also like to thank Faculty of Mechanical Engineering for their involvement and support during the project. We are as ever, especially indebted to our parents for their love and support throughout our lives. We also wish to thank our siblings for their support and understanding during our study. Moreover, our sincere thanks to our GIKIAN friends, who shared their love and experiences with us. Mohammad Usman Ehsan

Measure Angular Motion of a Mems-Based Gyroscope

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