Simulations of Simulations of Microgyroscope Microgyroscope Dynamics Dynamics
Oscar Vargas Oscar Vargas
Major: Mechanical Engineering Mentor: Laura Oropeza-Ramos Advisor: Kimberly L. Turner July 28, 2005
Simulations of Simulations of Microgyroscope Dynamics Dynamics - - PowerPoint PPT Presentation
Simulations of Simulations of Microgyroscope Dynamics Dynamics Microgyroscope Oscar Vargas Oscar Vargas Major: Mechanical Engineering Mentor: Laura Oropeza-Ramos Advisor: Kimberly L. Turner July 28, 2005 Goals of the research Goals of
Major: Mechanical Engineering Mentor: Laura Oropeza-Ramos Advisor: Kimberly L. Turner July 28, 2005
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Analyze non-
linear micro-
gyroscope dynamics through numerical simulations in MATLAB through numerical simulations in MATLAB
Understand MEMS principles
Reading from books, papers and discussions
Understand Linear and Nonlinear Micro-
gyroscopes
Dynamics of gyroscopes -
Coriolis effect effect
Study principles of vibration (parametric oscillation)
Use MATLAB
Create numerical simulations for different parameters values, mostly stiffness and mass values, mostly stiffness and mass
Microgyroscopes Microgyroscopes Microgyroscopes UCSB UCSB UCSB
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What is MEMS? Micro Electro-Mechanical Systems
Applications
Ships
Planes
Benefits of MEMS?
Low cost
Batch fabrication
Less material
Smaller – – Less Energy Less Energy
Less energy
Miniaturization
What is a gyroscope?
Macro-
gyroscope
Micro-
gyroscope
Microgyroscopes Microgyroscopes Microgyroscopes UCSB UCSB UCSB
Cars
Toys
http://www.bridgedeck.org http://www-bsac.eecs.berkeley.edu/archive/users/hui-elliot/mems.html
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Microgyroscopes Microgyroscopes Microgyroscopes UCSB UCSB UCSB
Robust Micromachined Vibratory Gyroscopes by Cenk Acar
m = mass c = damping F= external force Ω = angular velocity k = linear spring coefficient
Robust Micromachined Vibratory Gyroscopes by Cenk Acar
Ωz
z
x
y
A person looking at a ball traveling parallel to the y axis as he rotates
2 2
2
x x e z
d x dx dy m c k x F m dt dt dt + + = + Ω
2 2
2
y y z
d y dy dx m c k y m dt dt dt + + = − Ω
Coriolis effect Drawing of a micro-gyroscope Dynamics
2 ( )
c
F m v = ×Ω uu r r r
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Harmonic oscillation Parametric oscillation
Induced frequency response in a parametric gyroscopes Induced frequency response in a harmonic gyroscopes
Parametric resonance has a high amplitude for longer bandwidth Parametric resonance is less sensitive to changes in parameters thus gyro more robust
Robust Micromachined Vibratory Gyroscopes by Cenk Acar
Microgyroscopes Microgyroscopes Microgyroscopes UCSB UCSB UCSB
Non-interdigitated comb-fingers Interdigitated comb-fingers
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Amplitude in the x axis, actuated direction Amplitude in the y axis, induced direction Response in the x direction, driving direction Response in the y direction, sensing direction
Microgyroscopes Microgyroscopes Microgyroscopes UCSB UCSB UCSB
Displacement Frequency Response
0.00 1.00 2.00 3.00 4.00 5.00 6.00 7.00 8.00 9.00 10.00 18250 18350 18450 18550 18650 18750
Frequency(Hz) A m p litu d e (u m )
2m_1k
Displacement Frequency Responce
0.00E+00 2.00E-05 4.00E-05 6.00E-05 8.00E-05 1.00E-04 1.20E-04 18250 18350 18450 18550 18650 18750
Frequency(Hz) A m p litu d e (u m )
2m_1k
t
(Dimensionless)
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Microgyroscopes Microgyroscopes Microgyroscopes UCSB UCSB UCSB
Maximum amplitude vs. stiffness for different masses
Amplitude vs. Stiffness
0.00E+00 5.00E-05 1.00E-04 1.50E-04 2.00E-04 2.50E-04 5 10 15 20
Stiffness(N/m) Am plitude(um )
1m 2m 3m 4m m=0.275 ng
Structure of a micro-gyroscope
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Trevor Hirst Liu-Yen Kramer Nick Arnold Michael Northen Laura Oropeza-Ramos Kimberly L. Turner Turner group
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Ωz
z
x
y
A person looking at a ball traveling parallel to the y axis as he rotates
http://www.uvi.edu/SandM/Physics/dave/DavesArchives/111003 /Phys211NetPlay.html
Microgyroscopes Microgyroscopes Microgyroscopes UCSB UCSB UCSB
Foucault Pendulum swinging on the north pole
2 ( )
c
F m v = ×Ω uu r r r
Robust Micromachined Vibratory Gyroscopes by Cenk Acar
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3 2 1 3
( )
e
F r x r x V = − +
2 e
Non-interdigitated comb-fingers Interdigitated comb-fingers
x y x d
g
h
2 2
2
x x e z
d x dx dy m c k x F m dt dt dt + + = + Ω
2 2
2
y y z
d y dy dx m c k y m dt dt dt + + = − Ω
x