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1 EE C245 – ME C218 Introduction to MEMS Design F ll 200 Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley EE C245 : Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 1 University of California at Berkeley Berkeley, CA 94720 Lecture 15 : Beam Combos Lecture Outline Reading: Senturia, Chpt. 9 Lecture Topics: Bending of beams Bending of beams Cantilever beam under small deflections Combining cantilevers in series and parallel Folded suspensions Design implications of residual stress and stress gradients EE C245 : Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 2

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EE C245 – ME C218Introduction to MEMS Design

F ll 200Fall 2007

Prof. Clark T.-C. Nguyen

Dept. of Electrical Engineering & Computer SciencesUniversity of California at Berkeley

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 1

University of California at BerkeleyBerkeley, CA 94720

Lecture 15: Beam Combos

Lecture Outline

• Reading: Senturia, Chpt. 9• Lecture Topics:

Bending of beamsBending of beamsCantilever beam under small deflectionsCombining cantilevers in series and parallelFolded suspensionsDesign implications of residual stress and stress gradients

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 2

2

Stress Gradients in Cantilevers

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 3

Vertical Stress Gradients

• Variation of residual stress in the direction of film growth• Can warp released structures in z-direction

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 4

3

Stress Gradients in Cantilevers

• Below: surface micromachined cantilever deposited at a high temperature then cooled → assume compressive stress

Average stress

After

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 5

Stress gradient Once released, beam length increases slightly to relieve average stress

But stress gradient remains → induces moment that bends beam

which, stress is relieved

Stress Gradients in Cantilevers (cont)

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 6

4

Radius of Curvature f/ Stress Gradient

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 7

Measurement of Stress Gradient

• Use cantilever beamsStrain gradient (Γ = slope of stress-thickness curve) causes beams to deflect up or downAssuming linear strain gradient Γ, z = ΓL2/2g g ,

[P. Krulevitch Ph.D.]

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 8

5

Tip Bending Distance

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 9

Folded-Flexure Suspensions

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 10

6

Folded-Beam Suspension

• Use of folded-beam suspension brings many benefitsStress relief: folding truss is free to move in y-direction, so beams can expand and contract more readily to relieve stressHigh y-axis to x-axis stiffness ratio Folding Truss

x

y

z

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 11

Comb-Driven Folded Beam Actuator

Beam End Conditions

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 12

[From Reddy, Finite Element Method]

7

Common Loading & Boundary Conditions

• Displacement equations derived for various beams with concentrated load F or distributed load f

• Gary Fedder Ph.D. Thesis, EECS, UC Berkeley, 1994

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 13

Series Combinations of Springs

• For springs in series w/ one loadDeflections addSpring constants combine like “resistors in parallel”

x

y

z

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 14

8

Parallel Combinations of Springs

• For springs in parallel w/ one loadLoad is shared between the two springsSpring constant is the sum of the individual spring constants

x

y

z

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 15

Folded-Flexure Suspension Variants

• Below: just a subset of the different versions• All can be analyzed in a similar fashion

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 16

[From Michael Judy, Ph.D. Thesis, EECS, UC Berkeley, 1994]

9

Deflection of Folded Flexures

This equivalent to two cantilevers of

length Lc/2

Composite cantilever Composite cantilever free ends attach here

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 17

Half of F absorbed in other half

(symmetrical)4 sets of these pairs, each of

which gets ¼ of the total force F

Constituent Cantilever Spring Constant

• From our previous analysis:

( )yLEI

yFLyy

EILFyx c

z

c

cz

cc −=⎟⎟⎠

⎞⎜⎜⎝

⎛−= 3

631

2)(

22

zcz ⎠⎝

33

)( c

z

c

cc L

EILx

Fk ==

• From which the spring constant is:

• Inserting L = L/2

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 18

Inserting Lc = L/2

3324

)2/(3

LEI

LEI

k zzc ==

10

Overall Spring Constant

• Four pairs of clamped-guided beamsIn each pair, beams bend in series(Assume trusses are inflexible)

• Force is shared by each pair → Fpair = F/4

Rigid Truss

Force is shared by each pair → Fpair F/4

Leg

L

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 19

Fpair

Folded-Beam Stiffness Ratios

• In the x-direction:

• In the z direction:

Folded-beam suspension

324

LEI

k zx =

In the z-direction:Same flexure and boundary conditions

• In the y-direction:Shuttle

324

LEIk x

z =

EWh8

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 20

• Thus: Anchor

Folding truss

LEWhk y

8=

2

4 ⎟⎠⎞

⎜⎝⎛=WL

kk

x

yMuch

stiffer in y-direction!

[See Senturia, §9.2]

11

Folded-Beam Suspensions Permeate MEMS

Gyroscope [Draper Labs.]Accelerometer [ADXL-05, Analog Devices]

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 21

Micromechanical Filter [K. Wang, Univ. of Michigan]

Folded-Beam Suspensions Permeate MEMS

• Below: Micro-Oven Controlled Folded-Beam Resonator

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 22

12

Stressed Folded-Flexures

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 23

Clamped-Guided Beam Under Axial Load

• Important case for MEMS suspensions, since the thin films comprising them are often under residual stress

• Consider small deflection case: y(x) « Lxz

Governing differential equation: (Euler Beam Equation)

L

W

x

y

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 24

Governing differential equation: (Euler Beam Equation)

Unit impulse @ x=LAxial Load

13

The Euler Beam Equation

• Axial stresses produce no net horizontal force; but as soon as the beam is bent, there is a net downward force

For equilibrium, must postulate some kind of upward load on the beam to counteract the axial stress derived force

RAxial Stress

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 25

on the beam to counteract the axial stress-derived forceFor ease of analysis, assume the beam is bent to angle π

The Euler Beam Equation

Note: Use of the full bend angle of π to

establish conditions for load balance; but this returns us to case of

small displacements and small angles

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 26

14

Clamped-Guided Beam Under Axial Load

• Important case for MEMS suspensions, since the thin films comprising them are often under residual stress

• Consider small deflection case: y(x) « Lxz

Governing differential equation: (Euler Beam Equation)

L

W

x

y

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 27

Governing differential equation: (Euler Beam Equation)

Unit impulse @ x=LAxial Load

Solving the ODE

• Can solve the ODE using standard methodsSenturia, pp. 232-235: solves ODE for case of point load on a clamped-clamped beam (which defines B.C.’s)For solution to the clamped-guided case: see S. p gTimoshenko, Strength of Materials II: Advanced Theory and Problems, McGraw-Hill, New York, 3rd Ed., 1955

• Result from Timoshenko:

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 28

15

Design Implications

• Straight flexuresLarge tensile S means flexure behaves like a tensioned wire (for which k-1 = L/S)Large compressive S can lead to buckling (k-1 → ∞)g p g ( )

• Folded flexuresResidual stress only partially releasedLength from truss to shuttle’s centerline differs

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 29

centerline differs by Ls for inner and outer legs

Effect on Spring Constant

• Residual compression on outer legs with same magnitude of tension on inner legs:

⎟⎠⎞

⎜⎝⎛±=

LLs

rb εεBeam Strain: ; Stress Force: WhLLES s

r ⎟⎠⎞

⎜⎝⎛±= ε

• Spring constant becomes:⎠⎝ Lrb Lr

⎠⎝

EE C245: Introduction to MEMS Design Lecture 15 C. Nguyen 10/16/08 30

• Remedies:Reduce the shoulder width Ls to minimize stress in legsCompliance in the truss lowers the axial compression and tension and reduces its effect on the spring constant