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EE 570: Location and Navigation: Theory & Practice EE 570: Location and Navigation: Theory & Practice

EE 570: Location and Navigation: Theory & Practice - PowerPoint Presentation

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EE 570: Location and Navigation: Theory & Practice - PPT Presentation

Navigation Sensors and INS Mechanization Tuesday 12 Feb 2013 NMT EE 570 Location and Navigation Theory amp Practice Slide 1 of 19 Navigation Sensors and INS Mechanization Inertial Sensors ID: 199729

navigation sensors amp inertial sensors navigation inertial amp location theory practice 570 slide 2013 nmt tuesday feb mechanization ins

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Slide1

EE 570: Location and Navigation: Theory & Practice

Navigation Sensors and INS Mechanization

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Slide

1

of 19Slide2

Navigation Sensors and INS

Mechanization

Inertial Sensors

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

As the name implies inertial sensors measure motion

wrt

an inertial frame

Advantages: Self-contained & non-reliant on external fields (e.g. EM radiation, Earth’s magnetic field, …)Disadvantages: Typically rate measurements & expensiveAccelerometers measure linear accelerationActually measure specific force, typically, in the body frameGyroscopes measure angular velocityMost gyroscopes measure angular speed, typically, in the body frame

Slide

2

of 19Slide3

Navigation Sensors and INS Mechanization

Inertial Sensors

- Accelerometer

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Inertial Sensors

Accelerometers

Pendulous Mass

Vibratory

Closed

loop

Open

loop

Closed

loop

Open

loop

Gyroscopes

Slide

3

of 19Slide4

Navigation Sensors and INS Mechanization

Inertial

Sensors - Gyroscope

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Inertial Sensors

Gyroscopes

Rotating Mass

Sagnac

Effect

Coriolis Effect

Floated

DTG

Fluid Suspension

Magnetic Suspension

Mech

Suspension

Resonator

Interferometer

Ring Laser Gyro

Fiber Optic Gyro

Hemispherical Resonator Gyro

magnetohydrodynamic

Conductive fluid based

Microelectromechanical

Accelerometers

Slide

4

of 19Slide5

Navigation Sensors and INS Mechanization

Inertial Sensors – Accelerometer

: Pendulous Mass

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

The Pendulous Mass Accelerometer

A mass, a suspension system,

and a sensing element

Displacement  appliedforce resolved along thesensitive axis

Modeled as a basic 2nd order systemIn steady state

hence

 

Acceleration due to gravity

Reaction force

Mass

damper

k

spring

b

displacement (x)

Sense axis

Slide

5

of 19Slide6

Navigation Sensors and INS Mechanization

Inertial Sensors – Accelerometer: Pendulous Mass

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Closed-loop version generates a force to null the displacement

Can improve linearity and measurement range

Slide

6

of 19Slide7

Navigation Sensors and INS Mechanization

Inertial Sensors – Accelerometer: Pendulous Mass

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Pendulous Accelerometer

Closed loop configuration

Improved

linearity

Figure:

Clipp (2006)

Sensitive axis

Slide

7

of 19Slide8

Navigation Sensors and INS Mechanization

Inertial Sensors

– Accelerometer: Vibratory

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Vibratory accelerometers

Vibrating Beam Accelerometers (VBA)

Acceleration causes a change in resonance

frequency

Mass

Sensitive axis

Slide

8

of 19Slide9

Navigation Sensors and INS Mechanization

Inertial Sensors -

Accelerometer: Vibratory

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

MEMS Accelerometers

www.ett.bme.hu/memsedu

Slide

9

of 19Slide10

Navigation Sensors and INS Mechanization

Inertial Sensors -

Accelerometer: Vibratory

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

MEMS Accelerometers

Spring and mass from silicon and add fingers make a variable differential capacitor

Change in displacement => change in

capacitance

CS1 < CS2

APPLIED

ACCELERATION

SENSOR

ACCELERATING

MASS

SPRING

SENSOR AT REST

FIXED

ANCHOR TO

SUBSTRATE

Slide

10

of 19Slide11

Navigation Sensors and INS Mechanization

Inertial Sensors – Gyroscopes: Rotating Mass

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Rotating Mass Gyros

Conservation of Angular

Momentum

The spinning mass will resist

change in its angular momentumAngular momentumH = I  (Inertia * Angular velocity)By placing the gyro in a pair of frictionless gimbals it is free to maintain its inertial spin axisBy placing an index on the x-gimbal axes and y-gimbal axis two degrees of orientational motion can be

measured

Slide

11

of 19Slide12

Navigation Sensors and INS Mechanization

Inertial Sensors – Gyroscopes: Rotating Mass

Rotating Mass Gyros

PrecessionDisk is spinning about z-axis

Apply a torque about the x-axis

Results in precession about the y-axis

=

  H

x

y

z

Precession rate (

)

H(

t+dt

)

H(t)

dt

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Slide

12

of 19Slide13

Navigation Sensors and INS Mechanization

Inertial Sensors

– Gyroscopes:

Sagnac Effect Gyros

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Fiber

Optical Gyro (FOG)

Basic idea is that light travels at a constant speedIf rotated (orthogonal to the plane) one path length becomes longer and the other shorterThis is known as the Sagnac effect

Measuring path length change (over a dt) allows  to be measured

R

Detector

Transmitter

Slide

13

of 19Slide14

Navigation Sensors and INS Mechanization

Inertial Sensors -

Gyroscopes: Sagnac

Effect Gyros

Fiber Optical Gyro (FOG)

Measure the time difference

betw

the CW and CCW paths

CW transit time = tCWCCW transit time = tCCWLCW = 2R+Rt

CW = ctCWL

CCW = 2R-RtCCW

=

c

t

CCW

t

CW

= 2

R/(c-R

)

tCCW= 2R/(

c+R )With N turnsPhase

R

Splitter

Transmitter

Detector

R

Splitter

Transmitter

Detector

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Slide

14

of 19Slide15

Navigation Sensors and INS Mechanization

Inertial Sensors -

Gyroscopes: Sagnac

Effect GyrosTuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Ring Laser Gyro

A helium-neon laser produces two

light beams, one traveling in the

CW direction and the other in theCCW directionWhen rotatingThe wavelength in dir of rotationincreases (decrease in freq

)The wavelength in opposite dirdecreases (increase in freq)Similarly, it can be shown that

Slide

15

of 19Slide16

Navigation Sensors and INS Mechanization

Inertial Sensors - Gyroscopes: Coriolis

Effect

Vibratory Coriolis Angular Rate Sensor

Virtually all MEMS gyros are based on this

effect

Linear motion

Linear motion

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Slide

16

of 19Slide17

Navigation Sensors and INS Mechanization

Inertial Sensors - Gyroscopes: Coriolis Effect

Basic Planar Vibratory

Gyro

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Slide

17

of 19Slide18

Navigation Sensors and INS Mechanization

Inertial Sensors - Gyroscopes: Coriolis Effect

In plane sensing (left)

Out of plane sensing (right)

www.ett.bme.hu/memsedu

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Slide

18

of 19Slide19

Navigation Sensors and INS Mechanization

Inertial Sensors -

Summary

Tuesday 12 Feb 2013

NMT EE 570: Location and Navigation: Theory & Practice

Accelerometers

Measure specific force of the body frame

wrt

the inertial frame in the body frame coordinatesNeed to subtract the acceleration due to gravity to obtain the motion induced quantityIn general, all points on a rigid body do NOT experience the same linear velocityGyroscopesMeasure the inertial angular velocity Essentially, the rate of change of orientationAll points on a rigid body experience the same angular

velocity

Slide

19

of 19