CN100498803C - Reusable parameter module model building method for space continuous deformation MEMS - Google Patents

Reusable parameter module model building method for space continuous deformation MEMS Download PDF

Info

Publication number
CN100498803C
CN100498803C CNB2007100173053A CN200710017305A CN100498803C CN 100498803 C CN100498803 C CN 100498803C CN B2007100173053 A CNB2007100173053 A CN B2007100173053A CN 200710017305 A CN200710017305 A CN 200710017305A CN 100498803 C CN100498803 C CN 100498803C
Authority
CN
China
Prior art keywords
mems
equation
dynamic control
partiald
mems device
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
CNB2007100173053A
Other languages
Chinese (zh)
Other versions
CN101051328A (en
Inventor
马炳和
张承亮
吕湘连
苑伟政
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Northwestern Polytechnical University
Original Assignee
Northwestern Polytechnical University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Northwestern Polytechnical University filed Critical Northwestern Polytechnical University
Priority to CNB2007100173053A priority Critical patent/CN100498803C/en
Publication of CN101051328A publication Critical patent/CN101051328A/en
Application granted granted Critical
Publication of CN100498803C publication Critical patent/CN100498803C/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Micromachines (AREA)

Abstract

A modeling method of reusable parameterized component for space continuous deformation MEMS includes confirming each dynamic control equation and boundary condition equation of MEMS device, carrying out space discretization on dynamic control equation and converting said control equation to be constant-differential equation set, utilizing hardware description language of analog and mixed signal to carry out coding for realizing function description, plotting schematic diagram of MEMS device and connecting said diagram with code to form MEMS device being called in system modeling and in simulation analysis.

Description

The reusable parametrization assembly modeling method of space continuous modification MEMS
Technical field
The present invention relates to the method for establishing model of a kind of MEMS (micro electro mechanical system) (MEMS) device, belong to computer-aided design (CAD) (MEMS CAD) field of MEMS (micro electro mechanical system).
Background technology
Along with the raising of integrated level, the demand of MEMS system level design can be more and more urgent.System level design is paid close attention to whole micro-system (comprising physical construction, circuit and multiple domain coupling unit etc.) is carried out modeling and performance simulation on the whole.Because related work exists certain difficulty and complexity, therefore how to set up and can either more accurately express the device behavior and can realize that again reusable parametrization component model becomes key issue, for development MEMS cad technique, improve the MEMS design efficiency and the research and development level most important.
Nodal analysis can be set up the parametrization component model of MEMS device in the existing MEMS system-level modeling method, has obtained using widely.For example, the NODAS (Design ofActuators andSensors) of external Carnegie Mellon university exploitation, the SUGUR in the ARCHITECT of Coventor company, Berkeley branch school, University of California and the multiport three-dimensional micromodule modeling method of domestic Northwestern Polytechnical University etc. grows up on the nodal analysis basis basically.Its basic thought is that the device with labyrinth is decomposed into unit one by one, each unit is corresponding units corresponding storehouse respectively, be equivalent to primary element such as resistance, electric capacity and inductance etc. in the circuit, link to each other by node between the unit, and the quality and the rigidity of unit focused on the node deformation result the unknown between the node.Usually at the characteristics of MEMS device, system is divided into primary elements such as beam, stiffener plate, electrostatic gap, broach and anchor point.To primary element, methods such as apply materials mechanics and Structural Dynamics are set up the analytic model of lumped parameter.
Nodal analysis is by the end points concentrated reflection distortion situation of each MEMS functional structure.But for having space continuous modification behavior MEMS device, this method can not be described its deformational behavior in detail, i.e. the unknown as a result of the continuous modification in zone between the end points.In fact, most MEMS structure, as diaphragm, semi-girder, bridge etc., its deformational behavior all is that the space is continuous, these structures often relate to the height coupling of many physical domain such as static territory, domain, fluid territory, must obtain space continuous modification result to carry out directly related with it multiple domain coupling behavioural analysis.Therefore, at MEMS device, be necessary to set up special modeling method with space continuous modification behavioural characteristic.
Summary of the invention
Be not useable for describing deficiency in order to overcome prior art, the present invention proposes a kind of method for building up of the reusable parametrization component model at space continuous modification MEMS device with space continuous modification behavioural characteristic MEMS device.
The method for building up of the reusable parametrization component model of the space continuous modification MEMS device that the present invention proposes comprises the steps:
Step 1: energy territory and coupling scheme definite dynamic control equation, the boundary condition equation of describing each energy territory and couple state thereof thereof related according to the MEMS device.For most of MEMS devices such as semi-girder (single-ended fixing), bridge (two ends are fixed) and diaphragm (periphery is fixing) etc., owing to itself can not be approximately rigid body, its distortion has the continuous feature in space, so the dynamic control equation of such MEMS device is generally partial differential equation, its dynamic deformation amount is not only relevant with the time, and relevant with the locus.
Step 2: in conjunction with boundary condition, dynamic control equation to definite each the energy territory of description of step 1 carries out spatial discretization, on each Spatial Dimension, the MEMS device is carried out uniform grid and divide, replace partial differential with differential type then, thereby partial differential equation is converted to the ordinary differential equation group.
Step 3: according to the determined ordinary differential equation group of step 2, be input variable, adopt simulation and mixed signal hardware descriptive language (MAST, VHDL-AMS etc.) to encode, realize the functional description of device with MEMS size of devices parameter and technological parameter.
Step 4: draw MEMS assembly synoptic diagram, be connected, form the MEMS assembly, call during for system-level modeling and simulation analysis with coding.
Beneficial effect of the present invention has been to propose the method for building up of the reusable parametrization component model of a kind of space continuous modification MEMS device, and the component model that obtains can carry out system emulation with circuit.This method has reflected the basic characteristics of the space continuous modification that the many functional structures of MEMS are had, and the different types of reusable parametrization component model that has space continuous modification behavioral characteristic for foundation has directive function.For setting up models such as semi-girder, bridge, diaphragm fast, further make up the model of the device that comprises these unit or system and finish relevant overall permanence simulation analysis etc. easily and have important support effect.
The present invention is further described below in conjunction with drawings and Examples.
Description of drawings
Fig. 1: the system-level modeling process flow diagram of space continuous modification MEMS device.
Fig. 2: both-end is the little beam synoptic diagram of electrostatically actuated fixedly;
Among the figure, the 1-anchor point; The 2-bottom crown; The 3-substrate; The little beam of 4-.
Fig. 3: one-dimensional discrete process grid dividing figure.
Fig. 4: the little beam parametrization of electrostatically actuated assembly synoptic diagram.
Fig. 5: (a) vertical view of capacitance pressure transducer; (b) side view of capacitance pressure transducer.
Fig. 6: two-dimensional discrete process grid dividing figure.
Fig. 7: capacitance pressure transducer, parametrization assembly synoptic diagram.
Embodiment embodiment 1: the component model method for building up of the little beam of electrostatically actuated.
Step 1: energy territory and coupling scheme definite dynamic control equation, the boundary condition equation of describing each energy territory and couple state thereof thereof related according to the little beam of electrostatically actuated.
Accompanying drawing 2 is fixedly synoptic diagram of electrostatically actuated micro girder construction of a kind of both-end, and this structure is the common structure in the MEMS system, all is widely used in devices such as RF switch, micro-acceleration gauge, pressure transducer.When applying voltage V between upper/lower electrode, top electrode deforms under the effect of electrostatic attraction, and the amount of deflection that the size of the electrostatic force that each point is subjected on the beam is put therewith is relevant.The axis of beam when not being out of shape, promptly the straight line that is linked to be of each cross section centre of form is got and is made the x axle, does not consider the influence that rotate around neutral axis in detrusion and cross section.If the amount of deflection of beam each point is that (x, t), promptly the point at x place departs from the displacement of equilibrium position to w constantly on the beam at t.According to Euler's beam theory and static theory structure analysis being obtained the dynamic control equation of beam element under electrostatic force drives is:
EI ∂ 4 w ∂ x 4 - S ∂ 2 w ∂ x 2 + b ∂ w ∂ t + ρWh ∂ 2 w ∂ t 2 = - 1 2 ϵW V 2 ( t ) ( d + w ) 2 - - - ( 1 )
In the formula, L, W, h are respectively length, width and the thickness of beam, and d is an initial separation between pole plate.EI is called bendind rigidity, and E is the Young modulus of beam, and I is the moment of inertia of beam: I=Wh 3/ 12.
Boundary condition equation is:
w| x=0x=L=0
Figure C200710017305D00052
The electricity behavior of the little beam of electrostatically actuated can by under the description that establishes an equation:
i = dQ dt = dC dt V + C dV dt - - - ( 3 )
Wherein, Q is the quantity of electric charge of capacitor stores, and V is the voltage between two electrodes, and C is the electric capacity between the upper/lower electrode of beam distortion back:
C = ϵ ∫ x = 0 L W d + w ( x , y ) dx - - - ( 4 )
Step 2: in conjunction with boundary condition, dynamic control equation to definite each the energy territory of description of step 1 carry out one-dimensional discreteization, on each Spatial Dimension, the MEMS device is carried out uniform grid and divide, replace partial differential with differential type then, thereby partial differential equation is converted to the ordinary differential equation group.
At first must carry out discretize, be translated into the form of ordinary differential equation group partial differential equation (1), (2).Here adopt finite difference method, its process is that little beam is evenly divided grid, replaces partial differential with differential type then, and promptly the inclined to one side subitem of each node represents that with Centroid and its displacement of 4 nodes on every side as shown in Figure 3, used difference formula is as follows:
∂ w ∂ x ≈ 1 2 t ( w i + 1 - w i - 1 ) ∂ 2 w ∂ x 2 ≈ 1 t 2 ( w i - 1 - 2 w i + w i + 1 )
∂ 3 w ∂ x 3 ≈ 1 2 t 3 ( - w i - 2 + 2 w i - 1 - 2 w i + 1 + w i + 2 )
∂ 4 w ∂ x 4 ≈ 1 t 4 ( w i + 2 - 4 w i + 1 + 6 w i - 4 w i - 1 + w i - 2 )
Just can set up an equation at each node like this, thereby partial differential equation just is converted into the system equation that adopts the ordinary differential equation group to represent:
M w . . + K w . + Cw = F - - - ( 5 )
M wherein, K, C are system matrixes, w and F are amount of deflection and the load vectors that node (i) is located.
Step 3: according to the determined ordinary differential equation group of step 2, dimensional parameters and technological parameter with the little beam of electrostatically actuated are input variable, adopt simulation and mixed signal hardware descriptive language (MAST, VHDL-AMS etc.) to encode, realize the functional description of device.
Step 4: draw the little beam assembly synoptic diagram of electrostatically actuated, be connected, be embedded in the Component Gallery, for system-level calling with coding.The reusable parametrization assembly behavior model of the little beam of electrostatically actuated as shown in Figure 4.This assembly is made up of 4 ports, and two electric ports are top crown voltage v_t, and bottom crown voltage v_b, output port are capacitor C ap and central point displacement Z_mid.Structural parameters comprise the long L of little beam, wide W, and thick h, initial separation d etc. can pass through the graphical interfaces typing between pole plate.
Embodiment 2: the component model method for building up of capacitance pressure transducer.
Step 1: energy territory and coupling scheme definite dynamic control equation, the boundary condition equation of describing each energy territory and couple state thereof thereof related according to capacitance pressure transducer.
Accompanying drawing 5 is structural representations of a kind of capacitance pressure transducer,, and its flexible member is made of the diaphragm that props up admittedly all around.The deformation equation that diaphragm bears behind ambient pressure and the static pressure can be described as:
D ∂ 4 w ∂ x 4 + 2 D ∂ 4 w ∂ x 2 ∂ y 2 + D ∂ 4 w ∂ y 4 = p 0 + ϵ V 2 2 ( d - w ( x , y ) ) 2 - b dw dt - ρh d 2 w dt 2 - - - ( 6 )
Wherein: w is that (x, y are volume coordinates for x, displacement y), and D is bending stiffness D=Eh on the diaphragm 3/ 12/ (1-v 2), E is an elastic modulus, and v is a Poisson ratio, and ρ is a diaphragm density, and h is the thickness of diaphragm.
Boundary condition equation is:
w| x=0x=L=0
Figure C200710017305D00064
w| y=0y=L=0 (7)
The electricity behavior of capacitance pressure transducer, can by under the description that establishes an equation:
i = dQ dt = dC dt V + C dV dt - - - ( 8 )
Wherein, Q is the quantity of electric charge of capacitor stores, and V is the voltage between two electrodes, and C is the electric capacity behind the diaphragm deformation:
C = ϵ ∫ x = 0 L ∫ y = 0 W dxdy d - w ( x , y ) - - - ( 9 )
Step 2: in conjunction with boundary condition, dynamic control equation to definite each the energy territory of description of step 1 carry out two-dimensional discreteization, on each Spatial Dimension, the MEMS device is carried out uniform grid and divide, replace partial differential with differential type then, thereby partial differential equation is converted to the ordinary differential equation group.
At first must carry out discretize, be translated into the form of ordinary differential equation group partial differential equation (6), (7).Here adopt finite difference method, its process is that diaphragm is evenly divided grid, replaces partial differential with differential type then, and promptly the inclined to one side subitem of each node represents that with Centroid and its displacement of 12 nodes on every side as shown in Figure 6, used difference formula is as follows:
∂ w ∂ x ≈ 1 2 t ( w i + 1 , j - w i - 1 , j )
∂ 2 w ∂ x 2 ≈ 1 t 2 ( w i - 1 , j - 2 w i , j + w i + 1 , j )
∂ 4 w ∂ x 4 ≈ 1 t 4 ( w i + 2 , j - 4 w i + 1 , j + 6 w i , j - 4 w i - 1 , j + w i - 2 , j )
∂ 4 w ∂ x 2 ∂ y 2 ≈ 1 t 4 ( w i - 1 , j - 1 - 2 w i - 1 , j + w i - 1 , j + 1 - 2 w i , j - 1 + 4 w i , j - 2 w i , j + 1 + w i + 1 , j - 1 - 2 w i + 1 , j + w i + 1 , j + 1 )
Just can set up an equation at each node like this, thereby partial differential equation just is converted into the system equation that adopts the ordinary differential equation group to represent:
M w . . + K w . + Cw = F - - - ( 10 )
M wherein, K, C are system matrixes, w and F are node (i, amount of deflection of j) locating and load vectors.
Step 3: according to the determined ordinary differential equation group of step 2, dimensional parameters and technological parameter with capacitance pressure transducer, are input variable, adopt simulation and mixed signal hardware descriptive language (MAST, VHDL-AMS etc.) to encode, realize the functional description of device.
Step 4: draw capacitance pressure transducer, assembly synoptic diagram, be connected, be embedded in the Component Gallery, for system-level calling with coding.The reusable parametrization assembly behavior model of capacitance pressure transducer,, as shown in Figure 7.This assembly is made up of 5 ports, and input port is ambient pressure P, and two electric ports are top crown voltage V2, and bottom crown voltage V1, output port are capacitor C ap and central point displacement Z_mid.Structural parameters comprise the long L of diaphragm, wide W, and thick h, initial separation d etc. can pass through the graphical interfaces typing between pole plate.

Claims (1)

1, the reusable parametrization assembly modeling method of a kind of space continuous modification MEMS is characterized in that comprising the steps:
Step 1: energy territory and coupling scheme definite dynamic control equation, the boundary condition equation of describing each energy territory and couple state thereof thereof related according to the MEMS device;
Step 2: in conjunction with boundary condition, dynamic control equation to definite each the energy territory of description of step 1 carries out spatial discretization, on each Spatial Dimension the MEMS device being carried out uniform grid divides, replace partial differential with differential type then, thereby be dynamic control equation ordinary differential equation group form by the partial differential equation formal transformation;
Step 3: according to the determined ordinary differential equation group of step 2, be input variable, adopt simulation and mixed signal hardware descriptive language MAST or VHDL-AMS to encode, realize the functional description of device with MEMS size of devices parameter and technological parameter;
Step 4: draw MEMS assembly synoptic diagram, be connected, the MEMS assembly that calls when forming for system-level modeling and simulation analysis with coding.
CNB2007100173053A 2007-01-26 2007-01-26 Reusable parameter module model building method for space continuous deformation MEMS Expired - Fee Related CN100498803C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CNB2007100173053A CN100498803C (en) 2007-01-26 2007-01-26 Reusable parameter module model building method for space continuous deformation MEMS

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CNB2007100173053A CN100498803C (en) 2007-01-26 2007-01-26 Reusable parameter module model building method for space continuous deformation MEMS

Publications (2)

Publication Number Publication Date
CN101051328A CN101051328A (en) 2007-10-10
CN100498803C true CN100498803C (en) 2009-06-10

Family

ID=38782740

Family Applications (1)

Application Number Title Priority Date Filing Date
CNB2007100173053A Expired - Fee Related CN100498803C (en) 2007-01-26 2007-01-26 Reusable parameter module model building method for space continuous deformation MEMS

Country Status (1)

Country Link
CN (1) CN100498803C (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102004822B (en) * 2010-11-10 2012-10-31 哈尔滨工业大学 Modality-based frequency analysis method for space six-freedom-degree parallel motion system
US8762925B2 (en) * 2011-02-17 2014-06-24 Taiwan Semiconductor Manufacturing Company, Ltd. MEMS modeling system and method
CN103678066A (en) * 2013-12-18 2014-03-26 北京航天测控技术有限公司 Method and device for testing test signal set
WO2015152716A1 (en) * 2014-04-04 2015-10-08 Nederlandse Organisatie Voor Toegepast-Natuurwetenschappelijk Onderzoek Tno Actuator module for actuating a load
CN105677971B (en) * 2016-01-07 2018-11-30 郑州大学 Meet the square element deformation decomposition method of Complete Orthogonal and mechanical equilibrium condition
CN112190797B (en) * 2020-10-31 2022-07-01 河南省中医院(河南中医药大学第二附属医院) Department of anesthesia uses narcotic drug atomizer

Non-Patent Citations (6)

* Cited by examiner, † Cited by third party
Title
一种基于多端口组件网络的MEMS系统级建模方法. 霍鹏飞,马炳和,苑伟政.机械科学与技术,第24卷第2期. 2005
一种基于多端口组件网络的MEMS系统级建模方法. 霍鹏飞,马炳和,苑伟政.机械科学与技术,第24卷第2期. 2005 *
一种微构件的多物理场耦合求解方法. 张凯,彭云峰.机械设计与制造,第2期. 2006
一种微构件的多物理场耦合求解方法. 张凯,彭云峰.机械设计与制造,第2期. 2006 *
微机械系统建模与仿真技术研究. 季国顺,张永康.光学精密工程,第10卷第6期. 2006
微机械系统建模与仿真技术研究. 季国顺,张永康.光学精密工程,第10卷第6期. 2006 *

Also Published As

Publication number Publication date
CN101051328A (en) 2007-10-10

Similar Documents

Publication Publication Date Title
CN100498803C (en) Reusable parameter module model building method for space continuous deformation MEMS
CN110298105B (en) CCPDI-IMPM method for large deformation analysis of saturated porous medium
CN110795827B (en) Vortex-induced vibration simulation method for elastic support rigid cylinder structure under action of nonlinear energy well
CN100555294C (en) The whole-course numerical modeling method of main beam section pneumatic self excitation force
CN106295028A (en) A kind of partial structurtes dynamic modeling method and device
CN102566438A (en) Modelica language-based simulation modeling method of amplitude-changing mechanism of automobile crane
Bennini et al. Computational methods for reduced order modeling of coupled domain simulations
CN112329290A (en) Finite element discrete element multi-scale coupling calculation method for construction process simulation
CN103440386A (en) System and method for calculating driving torque of wind driven generator yaw system
CN109271655A (en) A kind of test-material yardstick effect analysis method based on asymmetric finite element algorithm
CN100570616C (en) The method for building up of micro-electromechanical variable cross-section clamped beam system-level macro model
CN103020406A (en) Data processing method and computer aided design system for shaft retaining structure
Telukunta et al. Fully Lagrangian modeling of MEMS with thin plates
CN1838133A (en) Concomitant engineering processing method in structure finite element computing
CN110334459B (en) Rapid and refined modeling system and method for power transmission tower line system
Iannacci et al. Compact modeling of a MEMS toggle-switch based on modified nodal analysis
Chen et al. Effects of monolithic silicon postulated as an isotropic material on design of microstructures
CN100430731C (en) Core kernel modeling method for micro inertial sensor device and core kernel base
Del Tin et al. Non linear compact modeling of RE-MEMS switches by means of model order reduction
Rochus et al. Non-conforming element for accurate modelling of MEMS
Wang et al. Genetic algorithm for electro-mechanical co-optimization of a MEMS accelerometer comprising a mechanical motion pre-amplifier with a 2nd-order sigma delta modulator
CN108073757B (en) Beam structure natural frequency analysis method based on power flow
CN103346251B (en) Segmented multilayer micro-cantilever piezoelectric actuator
Clement Dynamic Non-Linear Response of Owe Wave Energy Devices
Tsamados Fluid-solid interaction and modal analysis of a miniaturized piezoresistive pressure sensor

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20090610

Termination date: 20120126