This research deals with the effect of the intrinsic material length-scale parameter on the stability of a fully clamped rectangular micro-plate, which can be used as a RF MEMS resonator. A modified couple stress theory is utilized to model the micro-plate, considering the variable material length-scale parameter. The nonlinear governing equation of motion for static analysis is solved using the step-by-step linearization method (SSLM) and the static pull-in parameters, limiting the stable regions of capacitive resonators, are determined and compared to those obtained by the classical theory. The numerical results reveal that the intrinsic size dependence of materials leads to an increase in the pull-in voltage and natural frequency depending on the thickness of the micro-plate. Comparing these results to the experimental outcomes shows that utilizing the fixed material length-scale leads to unrealistic results in some manner.
3. Introduction
• RF MEMS
• Shapes of Actuators: Micro Beam, Rectangular or
Circular Micro-plate
• Pull-in Voltage
• Modified Couple Stress Theory (MCT)
• Material Length-scale parameter
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4. Research Background of RF MEMS
• Français and Dufour (1999)
proposed a complete normalized study of a diaphragm's behavior in MEMS and
compared the results with measurements made on silicon plates under
electrostatic actuation.
• Senturia (2000)
defined the structural instability phenomenon as “pull-in” in his book.
• Younis (2004)
presented an analysis and simulation of RF MEMS switches employing resonant
microbeams and investigated the pull-in instability and formulated safety criteria
for the design of MEMS sensors and RF filters in his Ph.D thesis.
• Talebian et al. (2010)
investigated the effect of temperature, stretching and residual stresses on the
static instability and natural frequency of an electrostatically actuated Kirchhoff
micro-plate using the classical theory (CT).
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5. Research Background of MCT
• Cosserat brothers (1909)
The Cosserat theory of elasticity incorporates the local rotation of points as well as
the translation allowed in CT. Moreover, there is a torque per unit area, or couple
stress, as well as the usual force per unit area, or stress.
• Yang et al. (2002)
The symmetric part of curvature tensor is an additional measure of deformation
that conjugates to the couple stress. This means that the number of required
material length scale parameters is only one in the modified couple stress theory
(MCT) instead of two in the classical couple stress theory (CCT).
• Tsiatas (2009)
A Kirchhoff plate model for the static analysis of isotropic micro-plates with
arbitrary shapes were derived based on MCT.
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7. Assumptions and Formulations
Lumped model
which are determined from the equalizing the static pull-in voltage and
first natural frequency of the mass-spring model with those obtained by
the distributed one.
and are the electrostatic and mass corrective coefficients, respectively,
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12. Numerical Solution
The micro-plate is at rest at equilibrium points ( ), hence these
points are obtained from
The order of this algebraic equation is three with respect to , which
depends on the DC voltage.
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Physically fixed points exist in , but mathematically, these
points might also exist in the range of .
17. Conclusions
• In the case of statically application of the voltage, the micro-plate goes
towards an unstable condition through a local saddle node bifurcation.
• Applying MCT shifts the saddle-node bifurcation point to a greater value.
• Based on the numerical results, the effect of material length-scale is
significant as the thickness becomes smaller.
• A fixed value for the material length-scale is not always realistic and
different problems require different values.
• Considering that the pull-in voltage and natural frequencies are directly
related to the plate rigidity, it is concluded that the obtained results for
the fundamental frequency using MCT are more realistic than those
obtained by CT.
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18. Thank you for your attention
On the Size-dependent Nonlinear Behavior of a Capacitive Rectangular Micro-plate
Considering Modified Couple Stress Theory
Kaveh Rashvand, Ghader Rezazadeh, Rasool Shabani, Mehrdad Sheikhlou
Mechanical Engineering Department
Editor's Notes
H
I am Kaveh Rashvand. I am going to present:
These are the outlines:
At the beginning, RF MEMS (radio frequency micro electro mechanical systems) refers to the application of MEMS technology to high frequency circuits in telecommunications, radar systems and cell phones.
Typical MEMS devices consist of a parallel-plate capacitor, in which one plate is actuated electrically and its motion is detected by capacitive changes. There are number of different actuator types at MEMS actuators, such as micro-beams, rectangular micro-plates, and circular micro-plates.
In RF MEMS devices, a microstructure is deflected by a DC bias voltage. It has been observed when the electrostatic forces is less than a critical value. After any disturbance, the flexible beam or plate of the system reaches a stable state. With increasing the applied voltage, the induced electrostatic forces overcome the existing forces so that the flexible part of the system deforms and collapses on the fixed electrode. This structural instability phenomenon is known as ‘pull-in’, and also the critical (minimum) voltage in which the pull-in phenomenon happens is called ‘pull-in voltage’.
The behavior of micro-scale structures has been observed experimentally to be size dependent. Therefore, the classical elasticity theory is not able to predict their responses properly.
According to the non-classical theory of elasticity, there is a torque per unit area, or couple stress, as well as the usual force per unit area, or stress in classical elasticity. These theories contain additional constants besides the Lamé constants which are difficult to determine named material length-scale parameter.
we can divide previous researches to two categories, first RF MEMS research area as shown here…
And second research area is non-classical theory:
Cosserat brothers presented their theory in 1909.
Young et al. modified cct in 2002.
And …… by Tsiatis in 2009.
our work utilizes MCT and actuated Tsiatas’s Kirchhoff plate by electrostatic load and compare the differences between the mechanical behaviors (pull-in voltage and natural frequency) of the plate and the Classical theory results.
D demonstrates the bending rigidity, Dl is the contribution of rotation gradient to the bending rigidity and q is the electrostatic pressure.
In order to simplify the analysis of the bifurcation behavior of the micro-plate, the distributed model is substituted by a lumped mass-spring model.
due to increase accuracy of the mass-spring model and adjusting this model with the distributed model, corrective coefficients are applied as a_zero and b_zero which are determined from the equalizing the static pull-in voltage and first natural frequency of the mass-spring model with those obtained by the distributed one.
For convenience following dimensionless parameters are defined for deflection, length, width and time:
Substituting dimensionless parameters to governing equations and dropping the hats, the non-dimensional static deflection equation arisen from statically applying the bias DC voltage, takes the following forms
This equation is nonlinear.
And the equation of mass-spring model is
By the governing equation nonlinearity, the analytical solution methods cannot be used to obtain the results; therefore, it is better to linearize the distibuted equation.
Rezazadeh et al. found SSLM in 2006 which proposed that the wi as a non-dimensional deflection of the micro-plate due to the applied DC voltage Vi.
By considering a small value for dv, it is expected that the Si would be small enough, hence for a suitable value of dv, it is possible to obtain desired accuracy.
Si can be approximated by truncating the summation series to finite numbers, and with respect to base functions of uppercase fi which is function of x and lowercase fi which function of y as
Applying the SSLM and using the Taylor’s series and its expansion to distributed model at i+1th step gives
This equation can be solved using the Galerkin Method
By multiplying R by fi fi as a weight function in the Galerkin method and integrating the outcome, a set of algebraic equations are obtained
Solving the set of M*N algebraic equations, the unknown mutipliers are calculated from
the multipliers are achieved through this equation from matrix AMN as the matrix of unknown coefficient and then the Si (dw) is calculated. Consequently, the static deflection of the micro-plate at each step of the applied voltage is determined.
At the equilibrium points (velocity equal zero), the micro-plate is at rest, hence considering Eq. (20) equilibrium points are obtained from this
To obtain these fixed points, following equation is solved
order of this algebraic equation is three with respect to which depends on the DC voltage
The following shape functions, which satisfy all boundary conditions for the rectangular micro-plate, are utilized
Pull-in voltage is calculated and obtained results are compared with the experimental results of Francais and Dufour. As shown in Figure, there is a very good agreement between the results.
It is worth mentioning that the micro-plate of Francais and Dufour was made of silicon, which has a small material length-scale parameter, therefore, the experimental and numerical results of the classical theory and MCT are very close to each other.
Cao et al. in 2007 reported values of gold length-scale parameter for different thicknesses. Therefore, in the present article, instead of a silicon micro-plate, a gold micro-plate is considered and the differences of the modified couple stress theory and classical theory has been investigated with this material and geometrical property.
As seen in this figure, for a given applied voltage (0<V<Vp ) three fixed points exist, but for V>Vp it decreases to one. In this Figure, stable centers and unstable saddle points are illustrated by solid and dashed curves, respectively. As shown, applying the modified couple stress theory shifts the saddle-node bifurcation point to right, and hence the calculated pull-in voltage increases from 2.301V to 3.864V.
This slide present motion trajectories of the gold micro-plate obtained from the modified couple stress theory for different values of applied voltage with different initial conditions.
for 0V and a voltage less than the pull-in voltage solid and dashed blue curves represent the periodic and unstable orbits, respectively. The black-bold curve represents the homoclinic orbit or boundary of attraction zone.
In 2.301 V and pull-in voltage figures show that increasing the applied voltage causes the basin of attraction of the physically stable center to be contracted, and when the applied voltage equals to the pull-in voltage there is no physically basin of attraction, and the system is unstable for every initial condition.
This figure shows the ratio of the static pull-in voltage calculated by the modified couple stress theory to the one calculated by the classical theory versus thickness. As seen, for lower values of the thickness the difference between two theories is significant, where increasing the thickness causes a decrease in the ratio of the pull-in voltage; while for thickness greater than 10 micron this ratio approaches 1. Furthermore, a fixed value of the material length-scale (that preposed by Zong and Soboyejo, 2005) is not always realistic and different problems could require different values (said by Voyiadjis and Abu Al-Rub, 2005).
Last fig. shows the variation of the non-dimensional fundamental frequency of the micro-plate versus applied DC voltage from zero to the pull-in voltage. As shown, the values of the fundamental frequency, for the micro-plate obtained by the modified couple stress theory (162 KHz and given voltage 0V), are greater than those obtained by classical theory (96 KHz and given voltage 0V).