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INTERNATIONAL JOURNAL OF COMPUTER ENGINEERING & 
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
TECHNOLOGY (IJCET) 
ISSN 0976 – 6367(Print) 
ISSN 0976 – 6375(Online) 
Volume 5, Issue 7, July (2014), pp. 73-84 
© IAEME: www.iaeme.com/IJCET.asp 
Journal Impact Factor (2014): 8.5328 (Calculated by GISI) 
www.jifactor.com 
73 
 
IJCET 
© I A E M E 
SIMULATED RF MEMS DOUBLE-POLE DOUBLE-THROW SWITCH 
USING A NOVEL SEESAW STRUCTURE 
Mohammed Al-Amin, Sufian Yousef, Barry Morris, Hassan Shirvani 
Anglia Ruskin University, Bishop Hall Lane, 
Chelmsford, Essex, CM1 1SQ, United Kingdom. 
 
ABSTRACT 
This paper explores the modelling and simulation of a Radio Frequency Micro Electro- 
Mechanical Systems (RF MEMS) switch using Finite Element modelling and analysis (FEM and 
FEA) tools on a novel seesaw design, providing Double-Pole Double-Throw (DPDT) functionality. 
This optimises the capabilities of the seesaw design structure for use in mobile communication 
systems and devices. After researching other available seesaw designs, it was realised that an 
improvement could be achieved by applying additional contacts within a 3D plane. 
During the development of the DPDT seesaw switch, a low electrostatic actuation voltage of 
14 V was achieved. This provided the switch with improved compatibility with voltages closer to 
those used in integrated circuits for mobile systems. 
The switch is a progression of existing Single-Pole Single-Throw (SPST) seesaw switches, 
with an additional set of upper and lower contacts at each end of the seesaw, offering DPDT 
switching capability within the space envelope. The length, height and width of the switch is 41 μm, 
7.6 μm and of 9 μm respectively, which is a suitable size for fabrication and conforms to the 
Microscale, from 1 μm to 100 μm. 
Copper Bulk General (Cu) was chosen for the pivot material on its merits of possessing good 
electrical conductivity and optimised flexibility and stiffness for elastic recovery. 
The simulation, using Intellisuite, attained a working switch design, with an ‘Air-Gap’ of 
1μm between the contacts, thus providing isolation when the switch is open-circuited. 
Keywords: DPDT, Electrostatic, Pivot, RF MEMS, Radio Frequency Micro Electro-Mechanical 
Systems, Seesaw, Simulated, Switch,
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
74 
1. INTRODUCTION 
 
As technology progresses, there is an ever increasing need for large-scale integration of RF 
MEMS switching devices within mobile communication systems. The aim of the research was to 
create a switch for mobile devices to allow switching between multiple different protocols or 
frequencies. The design also needed to have low power consumption for increased battery life and 
direct interfacing capabilities with mobile components, without additional circuitry. Achieving this 
leads to reduced cost and high reliability. With the use of RF MEMS switches, it is possible to meet 
all the criteria in a micro space envelope. 
Micro Electro-Mechanical Systems, also known as MEMS, is an emerging technology, which 
is finding its way into a number of applications, such as gyroscopes, sensors, digital imaging and 
mobile communications. The properties of materials change considerably from the macro-scale to 
the micro-scale. For example electrostatic forces become more significant, while the mass to surface 
area ratio becomes less significant. MEMS technology takes advantage of these small scale 
properties by being able to use simple electrostatic plates to develop actuation forces, and relatively 
increased surface area (with respect to mass) for heat dissipation, which in turn improves reliability. 
MEMS can be broken down into sub-fields, which include: 
MOEMS (Micro-Opto Electro-Mechanical Systems): used for optical imaging such as, digital light 
projection. 
Bio MEMS: an example of this is ‘Lab-on-a-Chip’ (LOC) where numerous biological tests can be 
carried out more efficiently than traditional testing techniques. 
MEMS Audio: used for microphonic sensors in commercial, studio microphones and mobile devices. 
MEMS Sensors: these include the detection of movement (in the x, y and z axes), heat, velocity and 
acceleration. 
RF MEMS: used for mobile phones, mobile base stations, satellites and other communication 
devices. 
Currently, MEMS devices are at a disadvantage when it comes to size constraints, as most RF 
MEMS switches are too large to be implemented into an integrated circuit and are packaged 
separately. This causes difficulty when creating smaller mobile devices. RF MEMS are commonly 
known for reliability issues [7] due to the moving components. There is a high chance of material 
fatigue and breakage [6], MEMS devices are also known to have a high voltage actuation (up to 
100V) [2, 8], which is due to electrostatic actuation and design size. This requires the device to 
provide a separate voltage source to be stepped up from a low voltage to a high voltage and causes 
the mobile device to consume more power than needed due the control circuitry and power 
conversion inefficiency. This paper takes these challenges into account, for the design of the RF 
MEMS switch, in order to overcome them. 
The paper concentrates on RF MEMS, more specifically, it addresses the use of RF MEMS 
switching on mobile phone devices with the goal to operate at lower voltages than those used in 
existing portable devices. The device was required to fit within the MEMS scale of 1 μm – 100 μm, 
with ease of fabrication for future integration into microchips.
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
75 
 
Figure 1: Cross sectional representation of the RF MEMS seesaw switch in the ‘off-state’ 
The research undertaken is a novel concept, using similar ideas of seesaw theory from K. 
Jongseok (2007) et al [4] and J. M. Cabral  A. S. Holmes (2006) [1]. These authors created an 
approach to design, with the seesaw concept, but as a Single- Pole Single-Throw (SPST) switch with 
similar voltages. The research in hand takes the SPST concept and adds addition contacts on a 3D 
plane. This provides the seesaw switch with Double-Pole Double-Throw (DPDT) connectivity and in 
turn gives the device the flexibility of selecting four protocols or frequencies. Multiple seesaw 
switches can be configured and utilised to provide an extensive switching selection of more than four 
configurations. This innovation has not been attempted, to date, and quadruples the connectivity 
within a reduced space envelope. 
The decision of using the seesaw concept over others, such as the wobble motor principle 
switch, designed by S. Pranonsatit (2006) et al [8], is that the design allows for multiple connectivity 
within a reduced area. Also, with the ability to reduce the size for lower actuation voltages. The 
wobble motor does provide Single-Pole 8-Throw (SP8T) switching, but sacrifices size and ease of 
fabrication, due to manually attaching the cartwheel. 
The procedure for development of the RF MEMS switch required the use of Finite Element 
Modelling (FEM) for designing the switch and Finite Element Analysis (FEA) for simulation. 
FEM modelling focuses on a two dimensional (2D) layout of the structure with the intent of 
creating a three dimensional (3D) design model. FEA simulation uses the FEM to provide stress, 
displacement and electromagnetic outcomes of the structure, for a given voltage input. 
The use of FEA software tools provides an expedient approach to design and simulation, 
while reducing cost to a minimum. These software tools can be used on a high specification 
computer to provide computational data of the structure of a MEMS device, without requiring 
external equipment or development time and cost. The software tools provide high precision analysis 
with regular updates. 
Intellisuite, created by Intellisense, was selected because of its software capabilities. It is able 
to provide a comprehensive materials database, efficient Solid and Process modelling tools and an 
effective Thermo-Electromechanical analysis tool [3] [5], with a graphical user interface (GUI) tool 
for users to develop and analyse MEMS devices. The software is designed for MEMS development 
only, but provides a simple CAD FEM tool with a validation tool to detect any errors in the mesh.
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
Intellisuite uses an intuitive method of designing, allowing the user to draw the shape on a grid with 
a mouse. 
76 
 
The properties of the materials used in MEMS are crucial to the functionality of the design, 
since the use of inappropriate materials can cause a malfunction or damage to the device and its 
peripheral components. Common materials used in RF MEMS simulations are Silicon Bulk General 
(Si), Copper Bulk General (Cu) and Aluminium Bulk General (Al) [2] [4]. 
The operating principles of this RF MEMS switch relies on an electrostatic force to close the 
contacts within an RF circuit (Figure 3). This force (F) depends on the following equation: 
 
 (1) 
Where, 
V = Supply voltage 
 = Dielectric constant of the ‘Air Gap’ 
A = Area of the electrostatic plates 
d = Distance between the electrostatic plates 
F = Force between the electrostatic plates 
Figure 2: Graphical representation of the force parameters 
The simulation takes into account fringe capacitance, which affects the forces on the beam. 
Fringe capacitance should be added to the equation as a constant (C) to provide improved accuracy 
to the result. The simulation required a voltage of 14 V to achieve a sufficient pulling force, using a 
copper pivot (Figure 6), with a pivot thickness of 0.0476 μm. The only parameters, which can be 
changed in equation 1, to increase this force, are the area (A) and the distance (d) between the 
parallel plates. As the seesaw is a symmetrical design, a degree of flexibility is required to ensure 
that the contacts on each side of the seesaw are closed simultaneously to provide maximum contact 
surface area, for a low resistance [4].
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
77 
 
Figure 3: Cross sectional representation of the activated RF MEMS seesaw switch in the ‘on-state’ 
The design, which has been created, incorporates most of the research developments within 
one structure, these are: low voltage actuation, reduced von-mises stress and increased switching 
functionally within a space envelope of the micrometre range. To understand the characteristics of 
the design, the research adopted an empirical, simulation based approach, in order to provide 
effective results, using Intellisuite software to model and simulate the RF MEMS seesaw switch. 
2. SUITABILITY OF THE DESIGN FOR MOBILE COMMUNICATION 
The research conducted has concentrated on optimising the best features of existing designs 
and incorporating them into a seesaw switch structure. The dimensions of the space envelope allows 
the design to be incorporated into mobile communication devices. RF MEMS provides innate 
advantages over conventional solid state switching materials; for example: 
• Low insertion loss, due to direct contact of low impedance materials 
• Low power consumption, due to voltage activation rather than current activation 
• Immunity to current leakage, due to no current path 
• High isolation, due to the ‘Air-Gap’ between contacts 
Compared to semiconductors, the ‘on-state’ resistance of RF MEMS is innately linear, 
because of its ohmic contacts. The seesaw mechanism relies on the elastic recovery forces of the 
pivot and is controlled by using two independent pull-down electrodes. 
3. DESIGN AND DEVELOPMENT 
To accommodate the Microscale between 1 μm to 100 μm, a length of 41 μm was chosen to 
be an appropriate value, enabling the design to be large enough to facilitate fabrication and small 
enough for increased switching speed. The distance between the beam contacts and the fixed 
contacts is 1 μm when in the ‘off-state’ (Figure 1). 
The seesaw pivot was designed using single polarity supply voltages across each pair of 
electrostatic plates, which were driven alternately with pulsed voltage waveforms. This allows 
reduced external control circuitry and circuit complexity. With the use of the DPDT switch design 
[1] [4], the RF MEMS seesaw device accommodates two distinct radio frequencies, which 
communicate simultaneously. By taking into account the area of the device (41 μm x 9 μm or 369 
μm2, which is shown in Table II), this increases functionality within the space envelope. With the 
use of elastic recovery, the device is set to the ‘off-state’ (Figure 1) without any voltages being 
applied.
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
78 
 
The pivot is the thinnest component of the structure, at a thickness of 0.0476 μm, which 
causes fabrication constraints. This restricts the design for use only with advanced fabrication 
techniques, such as 32 nm fabrication. The seesaw provides an advantage during the etching process 
because of its simple design, as it allows the etching solution to run though the structure without 
being held in the gaps. 
Table I: Seesaw Dimensions 
Seesaw Dimensions 
Elements Dimensions (μm) 
Air Gap 1 
Beam Length 41 
Beam Height 4 
Beam Width 5 
The seesaw RF MEMS switch enables switching between a dual input and output 
configuration, depending on the application. For primary use, it is configured for switching between 
two RX (receive) and TX (transmit) frequency bands. Other configurations may be used by 
employing RF mixers at the input to the seesaw RF MEMS switch, and provides simultaneous RX 
and TX for two distinct RF frequency bands. This in turn, provides a dual RX/TX switch with a total 
of four frequencies. The seesaw RF MEMS switch is designed to be used for mobile communication 
devices for common protocols such as GSM, Wi-Fi, 3G, 4G, WiMAX, Bluetooth, GPS and many 
other protocols. Depending on the capacity of the antennas, all protocols can be implemented, as 
most of them use frequencies that are less than 5.8 GHz. 
Figure 4: Activated RF MEMS seesaw switch. An earlier prototype simulation, of an oblique view 
in the ‘on-state’ with colour coded displacement 
The seesaw switch has the versatility of being connected into three configurations i.e. SPST 
DPDT or Single-Pole Double-Throw (SPDT) switching without any changes to the seesaw structure. 
This can be achieved by selecting the appropriate contact terminals. 
Using multiple RF MEMS seesaw switches with its three configurable modes, it is possible to 
achieve switching between multiple different protocols to create a switching matrix for GSM, 2G, 
3G, 4G, Bluetooth, Wi-Fi and GPS.
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
79 
4. TECHNIQUES OF THE SWITCH 
 
The RF MEMS device employs two SPDT switches, which are mounted at each end of a 
beam. The beam is balanced on a fixed central pivot to provide a seesaw mechanism. The pivot gives 
the seesaw elastic recovery of the beam, to a central position, when the switch is in the off-state. The 
pulling force, developed by the electrostatic plates, need to exceed the force of elastic recovery in 
order for the switch to make contact. During operation, each electrostatic plate is activated 
alternately to control the seesaw motion. Since the switches are mechanically linked via the beam, 
they are inversely synchronised with each other and may be considered as one Double-Pole Double- 
Throw (DPDT) switch. 
The seesaw motion of the beam is controlled by two complementary, electrostatic control 
signals, with a duty-cycle of 50 %, in the form of digital voltage pulses. The electrostatic forces, 
generated by these pulses, are used to alternately pull down each side of the seesaw to activate the 
switches. Four pairs of contact terminals are closed via the bridging contacts located at each end and 
both sides of the beam. Two switching pairs are closed simultaneously. This is shown in Figure 4. 
5. DESIGN PROCEDURE 
By looking at existing seesaw designs available, it was discovered that an improvement could 
be achieved by adding additional contacts. The SPST Seesaw switch [1] [4] could be improved to a 
DPDT switch by adding a set of upper and lower contacts to each side of the seesaw. 
One of the important design requirements for the seesaw switch is the pivot, as it is necessary 
for the switch to be used in three dimensions. In order to allow the beam to pivot in any orientation, 
consideration was given to the effect of gravity, even though this is relatively weak at the micro-scale. 
To keep in control of the movement, it is vital that the pivot is attached to the beam, for elastic 
recovery. 
Standard materials (silicon bulk general, copper bulk general and aluminium bulk general) 
were used from the Intellisense materials database. A number of database materials were tried and 
tested. Silicon bulk general, copper bulk general and aluminium bulk general were selected as ideal 
materials for use in MEMS fabrication. Silicon bulk general was used for all of the substrates and 
aluminium bulk general was used for the contacts and the electrostatic plates, as shown in Table II. 
For the pivot, two copper bulk general material thicknesses were considered, in order to evaluate 
their properties. The elastic recovery of the materials is an important property of the pivot to enable 
the ‘off-state’ of the switching to occur while providing flexibility for contact. 
Table II: Materials and beam specifications 
Materials 
Substrate (Si) Silicon Bulk General 
Pivot width 0.048 μm (Cu) Copper Bulk General 
Pivot width 0.053 μm 
(Cu) Copper Bulk General 
and 
(Al) Aluminium Bulk General 
Beam (Al) Aluminium Bulk General 
Contacts (Al) Aluminium Bulk General 
Electrostatic Plates (Al) Aluminium Bulk General
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
6. METHODOLOGY OF TESTING THE PARAMETERS 
80 
 
The technique of testing was by using Intellisense simulation software. The parameters of the 
simulation provides the electrostatic plates with controlled pulse-widths. If the beam did not respond 
to the pulse, the amplitude was then increased in increments, until the correct response in 
displacement was observed. 
The results were displayed graphically, by the simulation package, and the associated data 
exported into a Microsoft Excel spread-sheet for numerical analysis. This empirical approach to the 
research improved each area of the RF MEMS seesaw switch via multiple iterations, which yielded 
lower voltages and von mises stress levels. 
The waveforms have a mark-space ratio of 1:1 (equivalent to a duty cycle of 50%), which 
enables each side of the seesaw to be switched in an alternating fashion. 
7. EXPERIMENTAL ANALYSIS 
Using Thermo Electro-Mechanical analysis, a set of dynamic results were produced (Figures 
6-8). This uses time, stress and displacement data to provide the seesaw switch with a time based 
movement. 
Figure 5 shows that the displacement of the beam reaches 1 μm (thus enabling the contacts to 
close) when a voltage of 14 volts was applied across the electrostatic plates, for copper, using static 
simulation for a ranged voltage analysis. 
Figure 5: Static analysis of displacement vs. Voltage for copper with a width of 0.048 μm 
This displacement is also shown in Figure 6 and Figure 7 as a function of time with pivot 
widths of 0.048 μm and 0.053 μm, respectively. The 0.053 μm thick pivot does not allow sufficient 
displacement due to its stiffness and prevents the contacts from closing.
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
Figure 6: Dynamic analysis of displacement vs. Time using a copper pivot with a width of 0.048 μm 
Figure 7: Dynamic analysis of displacement vs. Time using a copper pivot with a width of 0.053 μm 
81 
 
Figure 8 also shows a graph of displacement of the beam as a function of time, using 
aluminium. Although aluminium has the same pivot thickness of 0.053 μm as the copper pivot 
shown in Figure 7, it provided a displacement which reached its target destination due to the innate 
flexibility of the material. 
Figure 8: Dynamic analysis of displacement vs. Time using an Aluminium pivot with a width of 
0.053 μm
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
82 
 
A dynamic simulation was carried out using aluminium with a pivot thickness of 0.048 μm, 
however, the software reported that the aluminium pivot material exceeded its boundary conditions 
and failed, therefore no graph was produced. 
A separate experiment was conducted for the thickness of the pivot. Figures 9 and 10 show 
von mises stress and displacement vs the thickness of the aluminium and copper materials 
respectively, with a pulling voltage of 3 V. 
The experiments show aluminium to provide higher flexibility over copper at a thickness of 
0.05μm, but compromises von mises stress that goes beyond its ultimate yield strength, which would 
lead to fracture failure. 
Copper provides an optimum displacement at the same thickness, with a von mises stress 
under the yield strength, which guarantees no deformity of the material during the electrostatic 
pulling force. Therefore, copper bulk general was selected as the pivot material, because of its 
intrinsic properties. 
Figure 9: Von Mises Stress and Displacement vs Thickness of Aluminium pivot at 3V 
Figure 10: Von Mises Stress and Displacement vs Thickness of Copper pivot at 3V
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
83 
8. CONCLUSION 
 
After numerous iterations of the design, the electrostatic supply voltage was reduced 
significantly from typical values exceeding 40 volts to 14 volts for copper bulk general. This was 
achieved using empirical analysis to observe each area of the structure for improvements. 
The maximum pulling force was achieved by making use of the surface area of the 
electrostatic plates on the beam and the base of the seesaw. Also, an improvement was made by 
optimising the thickness of the pivot to operate under von mises stress and applying the minimum 
voltage for increased reliability. 
A working simulation was achieved without compromising the ‘Air-Gap’ between the 
contacts, which retained isolation when the switch was open-circuited, with alternating pulses. By 
using dynamic analysis on Intellisuite software, the seesaw action was enabled. 
The seesaw RF MEMS switch is an improved concept over existing designs, which are 
limited to Single-Pole Single-Throw (SPST) switching [1] 
[4]. Additional contacts, in the improved design, achieve DPDT switching, and required lower 
actuation voltages, due to the reduction in size. 
The seesaw switch may be configured into three switching modes (SPST, SPDT and DPDT) making 
it a versatile component for use within integrated circuits for mobile communication devices. 
9. ACKNOWLEDGMENT 
The authors’ acknowledgment is given to Jianhua Mao from Intellisense for his software 
support and valuable advice on Intellisuite modelling and simulation software tools. 
10. REFERENCES 
[1] J. M CABRAL  A.S. HOLMES, (2006). “A novel seesaw-type RF MEMS switch.” 
Electrotechnical Conference, 2006. MELECON 2006, IEEE Mediterranean 2006, pp. 288- 
292. 
[2] K.HYOUK, C. DONG-JUNE, P.AE-HYOUNG, L. HEE-CHUL, P. YONG-HEE, K. YONG-DAE, 
N. HYO-JIN, J. YOUNG-CHANG  B. JONG-UK (2007). “Contact materials and 
reliability for high power RF-MEMS switches.” Micro Electro Mechanical Systems, 2007. 
MEMS. IEEE 20th International Conference on 2007, pp. 231-234. 
[3] H. JAAFAR, N. FONG LI  N.A.M. YUNUS (2011). “Design and simulation of high 
performance RF MEMS series switch.” Micro and Nanoelectronics (RSM), 2011 IEEE 
Regional Symposium on 2011, pp. 349-353. 
[4] K.JONGSEOK, K. SANGWOOK, Y. HONG, J. HEEMOON  L. SANGHOON (2007). 
“Variable pivot seesaw actuated RF MEMS switch for reconfigurable system application.” 
Micro Electro Mechanical Systems, 2007. MEMS. IEEE 20th International Conference on 
2007, pp. 775-778. 
[5] A.M. PASHA  M.A. SAQIB (2009). “Design optimization for low voltage DC contact RF 
MEMS shunt switch.” Electrical Engineering, 2009. ICEE '09. Third International 
Conference on 2009, pp. 1-6. 
[6] H. R. Shea (2006), “Reliability of MEMS for space applications” Proc. of SPIE Reliability, 
Packaging, Testing, and Characterization of MEMS/MOEMS V on 2006, vol. Vol. 6111, 
61110A. 
[7] J. HWANG, 2007. “Reliability of Electrostatically Actuated RF MEMS Switches” Radio- 
Frequency Integration Technology, 2007. RFIT 007. IEEE International Workshop on 2007, 
pp. 168-171.
International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), 
ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 
84 
 
[8] S. PRANONSATIT, G. HONG, A.S. HOLMES and S. LUCYSZYN, 2006. “Rotary RF 
MEMS Switch Based on the Wobble Motor Principle” Micro Electro Mechanical Systems, 
2006. MEMS 2006 Istanbul. 19th IEEE International Conference on 2006, pp. 886-889. 
[9] Anesh K Sharma, Ashu K Gautam, CG Balaji, Asudeb Dutta and SG Singh, 2012. “Shunt Rf 
Mems Switch with Low Potential and Low Losson Quartz for Reconfigurable Circuit 
Applications”, International Journal of Electronics and Communication Engineering  
Technology (IJECET), Volume 3, Issue 2, pp. 497 - 510, ISSN Print: 0976- 6464, 
ISSN Online: 0976 –6472. 
11. ABBREVIATIONS 
2G Second Generation 
3G Third Generation 
4G Fourth Generation 
BIO MEMS Biological Micro Electro- 
Mechanical Systems 
DC Direct Current 
DPDT Double-Pole-Double-Throw 
GHz Giga-Hertz 
GPS Global Positioning System 
GSM Global System for Mobile 
Communications 
MEMS Micro Electro-Mechanical 
Systems 
MOMEMS Micro-Opto Electro- 
Mechanical Systems 
ms Milliseconds 
SPDT Single-Pole Double-Throw 
SPST Single-Pole Single-Throw 
SP8T Single-Pole Eight-Throw 
RX Receive 
RF MEMS Radio Frequency Micro 
Electro-Mechanical Systems 
TX Transmit 
μm Micrometre 
Wi-Fi Wireless Fidelity 
WiMAX Worldwide Interoperability for 
Microwave Access

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  • 1. INTERNATIONAL JOURNAL OF COMPUTER ENGINEERING & International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME TECHNOLOGY (IJCET) ISSN 0976 – 6367(Print) ISSN 0976 – 6375(Online) Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME: www.iaeme.com/IJCET.asp Journal Impact Factor (2014): 8.5328 (Calculated by GISI) www.jifactor.com 73 IJCET © I A E M E SIMULATED RF MEMS DOUBLE-POLE DOUBLE-THROW SWITCH USING A NOVEL SEESAW STRUCTURE Mohammed Al-Amin, Sufian Yousef, Barry Morris, Hassan Shirvani Anglia Ruskin University, Bishop Hall Lane, Chelmsford, Essex, CM1 1SQ, United Kingdom. ABSTRACT This paper explores the modelling and simulation of a Radio Frequency Micro Electro- Mechanical Systems (RF MEMS) switch using Finite Element modelling and analysis (FEM and FEA) tools on a novel seesaw design, providing Double-Pole Double-Throw (DPDT) functionality. This optimises the capabilities of the seesaw design structure for use in mobile communication systems and devices. After researching other available seesaw designs, it was realised that an improvement could be achieved by applying additional contacts within a 3D plane. During the development of the DPDT seesaw switch, a low electrostatic actuation voltage of 14 V was achieved. This provided the switch with improved compatibility with voltages closer to those used in integrated circuits for mobile systems. The switch is a progression of existing Single-Pole Single-Throw (SPST) seesaw switches, with an additional set of upper and lower contacts at each end of the seesaw, offering DPDT switching capability within the space envelope. The length, height and width of the switch is 41 μm, 7.6 μm and of 9 μm respectively, which is a suitable size for fabrication and conforms to the Microscale, from 1 μm to 100 μm. Copper Bulk General (Cu) was chosen for the pivot material on its merits of possessing good electrical conductivity and optimised flexibility and stiffness for elastic recovery. The simulation, using Intellisuite, attained a working switch design, with an ‘Air-Gap’ of 1μm between the contacts, thus providing isolation when the switch is open-circuited. Keywords: DPDT, Electrostatic, Pivot, RF MEMS, Radio Frequency Micro Electro-Mechanical Systems, Seesaw, Simulated, Switch,
  • 2. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 74 1. INTRODUCTION As technology progresses, there is an ever increasing need for large-scale integration of RF MEMS switching devices within mobile communication systems. The aim of the research was to create a switch for mobile devices to allow switching between multiple different protocols or frequencies. The design also needed to have low power consumption for increased battery life and direct interfacing capabilities with mobile components, without additional circuitry. Achieving this leads to reduced cost and high reliability. With the use of RF MEMS switches, it is possible to meet all the criteria in a micro space envelope. Micro Electro-Mechanical Systems, also known as MEMS, is an emerging technology, which is finding its way into a number of applications, such as gyroscopes, sensors, digital imaging and mobile communications. The properties of materials change considerably from the macro-scale to the micro-scale. For example electrostatic forces become more significant, while the mass to surface area ratio becomes less significant. MEMS technology takes advantage of these small scale properties by being able to use simple electrostatic plates to develop actuation forces, and relatively increased surface area (with respect to mass) for heat dissipation, which in turn improves reliability. MEMS can be broken down into sub-fields, which include: MOEMS (Micro-Opto Electro-Mechanical Systems): used for optical imaging such as, digital light projection. Bio MEMS: an example of this is ‘Lab-on-a-Chip’ (LOC) where numerous biological tests can be carried out more efficiently than traditional testing techniques. MEMS Audio: used for microphonic sensors in commercial, studio microphones and mobile devices. MEMS Sensors: these include the detection of movement (in the x, y and z axes), heat, velocity and acceleration. RF MEMS: used for mobile phones, mobile base stations, satellites and other communication devices. Currently, MEMS devices are at a disadvantage when it comes to size constraints, as most RF MEMS switches are too large to be implemented into an integrated circuit and are packaged separately. This causes difficulty when creating smaller mobile devices. RF MEMS are commonly known for reliability issues [7] due to the moving components. There is a high chance of material fatigue and breakage [6], MEMS devices are also known to have a high voltage actuation (up to 100V) [2, 8], which is due to electrostatic actuation and design size. This requires the device to provide a separate voltage source to be stepped up from a low voltage to a high voltage and causes the mobile device to consume more power than needed due the control circuitry and power conversion inefficiency. This paper takes these challenges into account, for the design of the RF MEMS switch, in order to overcome them. The paper concentrates on RF MEMS, more specifically, it addresses the use of RF MEMS switching on mobile phone devices with the goal to operate at lower voltages than those used in existing portable devices. The device was required to fit within the MEMS scale of 1 μm – 100 μm, with ease of fabrication for future integration into microchips.
  • 3. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 75 Figure 1: Cross sectional representation of the RF MEMS seesaw switch in the ‘off-state’ The research undertaken is a novel concept, using similar ideas of seesaw theory from K. Jongseok (2007) et al [4] and J. M. Cabral A. S. Holmes (2006) [1]. These authors created an approach to design, with the seesaw concept, but as a Single- Pole Single-Throw (SPST) switch with similar voltages. The research in hand takes the SPST concept and adds addition contacts on a 3D plane. This provides the seesaw switch with Double-Pole Double-Throw (DPDT) connectivity and in turn gives the device the flexibility of selecting four protocols or frequencies. Multiple seesaw switches can be configured and utilised to provide an extensive switching selection of more than four configurations. This innovation has not been attempted, to date, and quadruples the connectivity within a reduced space envelope. The decision of using the seesaw concept over others, such as the wobble motor principle switch, designed by S. Pranonsatit (2006) et al [8], is that the design allows for multiple connectivity within a reduced area. Also, with the ability to reduce the size for lower actuation voltages. The wobble motor does provide Single-Pole 8-Throw (SP8T) switching, but sacrifices size and ease of fabrication, due to manually attaching the cartwheel. The procedure for development of the RF MEMS switch required the use of Finite Element Modelling (FEM) for designing the switch and Finite Element Analysis (FEA) for simulation. FEM modelling focuses on a two dimensional (2D) layout of the structure with the intent of creating a three dimensional (3D) design model. FEA simulation uses the FEM to provide stress, displacement and electromagnetic outcomes of the structure, for a given voltage input. The use of FEA software tools provides an expedient approach to design and simulation, while reducing cost to a minimum. These software tools can be used on a high specification computer to provide computational data of the structure of a MEMS device, without requiring external equipment or development time and cost. The software tools provide high precision analysis with regular updates. Intellisuite, created by Intellisense, was selected because of its software capabilities. It is able to provide a comprehensive materials database, efficient Solid and Process modelling tools and an effective Thermo-Electromechanical analysis tool [3] [5], with a graphical user interface (GUI) tool for users to develop and analyse MEMS devices. The software is designed for MEMS development only, but provides a simple CAD FEM tool with a validation tool to detect any errors in the mesh.
  • 4. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME Intellisuite uses an intuitive method of designing, allowing the user to draw the shape on a grid with a mouse. 76 The properties of the materials used in MEMS are crucial to the functionality of the design, since the use of inappropriate materials can cause a malfunction or damage to the device and its peripheral components. Common materials used in RF MEMS simulations are Silicon Bulk General (Si), Copper Bulk General (Cu) and Aluminium Bulk General (Al) [2] [4]. The operating principles of this RF MEMS switch relies on an electrostatic force to close the contacts within an RF circuit (Figure 3). This force (F) depends on the following equation: (1) Where, V = Supply voltage = Dielectric constant of the ‘Air Gap’ A = Area of the electrostatic plates d = Distance between the electrostatic plates F = Force between the electrostatic plates Figure 2: Graphical representation of the force parameters The simulation takes into account fringe capacitance, which affects the forces on the beam. Fringe capacitance should be added to the equation as a constant (C) to provide improved accuracy to the result. The simulation required a voltage of 14 V to achieve a sufficient pulling force, using a copper pivot (Figure 6), with a pivot thickness of 0.0476 μm. The only parameters, which can be changed in equation 1, to increase this force, are the area (A) and the distance (d) between the parallel plates. As the seesaw is a symmetrical design, a degree of flexibility is required to ensure that the contacts on each side of the seesaw are closed simultaneously to provide maximum contact surface area, for a low resistance [4].
  • 5. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 77 Figure 3: Cross sectional representation of the activated RF MEMS seesaw switch in the ‘on-state’ The design, which has been created, incorporates most of the research developments within one structure, these are: low voltage actuation, reduced von-mises stress and increased switching functionally within a space envelope of the micrometre range. To understand the characteristics of the design, the research adopted an empirical, simulation based approach, in order to provide effective results, using Intellisuite software to model and simulate the RF MEMS seesaw switch. 2. SUITABILITY OF THE DESIGN FOR MOBILE COMMUNICATION The research conducted has concentrated on optimising the best features of existing designs and incorporating them into a seesaw switch structure. The dimensions of the space envelope allows the design to be incorporated into mobile communication devices. RF MEMS provides innate advantages over conventional solid state switching materials; for example: • Low insertion loss, due to direct contact of low impedance materials • Low power consumption, due to voltage activation rather than current activation • Immunity to current leakage, due to no current path • High isolation, due to the ‘Air-Gap’ between contacts Compared to semiconductors, the ‘on-state’ resistance of RF MEMS is innately linear, because of its ohmic contacts. The seesaw mechanism relies on the elastic recovery forces of the pivot and is controlled by using two independent pull-down electrodes. 3. DESIGN AND DEVELOPMENT To accommodate the Microscale between 1 μm to 100 μm, a length of 41 μm was chosen to be an appropriate value, enabling the design to be large enough to facilitate fabrication and small enough for increased switching speed. The distance between the beam contacts and the fixed contacts is 1 μm when in the ‘off-state’ (Figure 1). The seesaw pivot was designed using single polarity supply voltages across each pair of electrostatic plates, which were driven alternately with pulsed voltage waveforms. This allows reduced external control circuitry and circuit complexity. With the use of the DPDT switch design [1] [4], the RF MEMS seesaw device accommodates two distinct radio frequencies, which communicate simultaneously. By taking into account the area of the device (41 μm x 9 μm or 369 μm2, which is shown in Table II), this increases functionality within the space envelope. With the use of elastic recovery, the device is set to the ‘off-state’ (Figure 1) without any voltages being applied.
  • 6. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 78 The pivot is the thinnest component of the structure, at a thickness of 0.0476 μm, which causes fabrication constraints. This restricts the design for use only with advanced fabrication techniques, such as 32 nm fabrication. The seesaw provides an advantage during the etching process because of its simple design, as it allows the etching solution to run though the structure without being held in the gaps. Table I: Seesaw Dimensions Seesaw Dimensions Elements Dimensions (μm) Air Gap 1 Beam Length 41 Beam Height 4 Beam Width 5 The seesaw RF MEMS switch enables switching between a dual input and output configuration, depending on the application. For primary use, it is configured for switching between two RX (receive) and TX (transmit) frequency bands. Other configurations may be used by employing RF mixers at the input to the seesaw RF MEMS switch, and provides simultaneous RX and TX for two distinct RF frequency bands. This in turn, provides a dual RX/TX switch with a total of four frequencies. The seesaw RF MEMS switch is designed to be used for mobile communication devices for common protocols such as GSM, Wi-Fi, 3G, 4G, WiMAX, Bluetooth, GPS and many other protocols. Depending on the capacity of the antennas, all protocols can be implemented, as most of them use frequencies that are less than 5.8 GHz. Figure 4: Activated RF MEMS seesaw switch. An earlier prototype simulation, of an oblique view in the ‘on-state’ with colour coded displacement The seesaw switch has the versatility of being connected into three configurations i.e. SPST DPDT or Single-Pole Double-Throw (SPDT) switching without any changes to the seesaw structure. This can be achieved by selecting the appropriate contact terminals. Using multiple RF MEMS seesaw switches with its three configurable modes, it is possible to achieve switching between multiple different protocols to create a switching matrix for GSM, 2G, 3G, 4G, Bluetooth, Wi-Fi and GPS.
  • 7. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 79 4. TECHNIQUES OF THE SWITCH The RF MEMS device employs two SPDT switches, which are mounted at each end of a beam. The beam is balanced on a fixed central pivot to provide a seesaw mechanism. The pivot gives the seesaw elastic recovery of the beam, to a central position, when the switch is in the off-state. The pulling force, developed by the electrostatic plates, need to exceed the force of elastic recovery in order for the switch to make contact. During operation, each electrostatic plate is activated alternately to control the seesaw motion. Since the switches are mechanically linked via the beam, they are inversely synchronised with each other and may be considered as one Double-Pole Double- Throw (DPDT) switch. The seesaw motion of the beam is controlled by two complementary, electrostatic control signals, with a duty-cycle of 50 %, in the form of digital voltage pulses. The electrostatic forces, generated by these pulses, are used to alternately pull down each side of the seesaw to activate the switches. Four pairs of contact terminals are closed via the bridging contacts located at each end and both sides of the beam. Two switching pairs are closed simultaneously. This is shown in Figure 4. 5. DESIGN PROCEDURE By looking at existing seesaw designs available, it was discovered that an improvement could be achieved by adding additional contacts. The SPST Seesaw switch [1] [4] could be improved to a DPDT switch by adding a set of upper and lower contacts to each side of the seesaw. One of the important design requirements for the seesaw switch is the pivot, as it is necessary for the switch to be used in three dimensions. In order to allow the beam to pivot in any orientation, consideration was given to the effect of gravity, even though this is relatively weak at the micro-scale. To keep in control of the movement, it is vital that the pivot is attached to the beam, for elastic recovery. Standard materials (silicon bulk general, copper bulk general and aluminium bulk general) were used from the Intellisense materials database. A number of database materials were tried and tested. Silicon bulk general, copper bulk general and aluminium bulk general were selected as ideal materials for use in MEMS fabrication. Silicon bulk general was used for all of the substrates and aluminium bulk general was used for the contacts and the electrostatic plates, as shown in Table II. For the pivot, two copper bulk general material thicknesses were considered, in order to evaluate their properties. The elastic recovery of the materials is an important property of the pivot to enable the ‘off-state’ of the switching to occur while providing flexibility for contact. Table II: Materials and beam specifications Materials Substrate (Si) Silicon Bulk General Pivot width 0.048 μm (Cu) Copper Bulk General Pivot width 0.053 μm (Cu) Copper Bulk General and (Al) Aluminium Bulk General Beam (Al) Aluminium Bulk General Contacts (Al) Aluminium Bulk General Electrostatic Plates (Al) Aluminium Bulk General
  • 8. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 6. METHODOLOGY OF TESTING THE PARAMETERS 80 The technique of testing was by using Intellisense simulation software. The parameters of the simulation provides the electrostatic plates with controlled pulse-widths. If the beam did not respond to the pulse, the amplitude was then increased in increments, until the correct response in displacement was observed. The results were displayed graphically, by the simulation package, and the associated data exported into a Microsoft Excel spread-sheet for numerical analysis. This empirical approach to the research improved each area of the RF MEMS seesaw switch via multiple iterations, which yielded lower voltages and von mises stress levels. The waveforms have a mark-space ratio of 1:1 (equivalent to a duty cycle of 50%), which enables each side of the seesaw to be switched in an alternating fashion. 7. EXPERIMENTAL ANALYSIS Using Thermo Electro-Mechanical analysis, a set of dynamic results were produced (Figures 6-8). This uses time, stress and displacement data to provide the seesaw switch with a time based movement. Figure 5 shows that the displacement of the beam reaches 1 μm (thus enabling the contacts to close) when a voltage of 14 volts was applied across the electrostatic plates, for copper, using static simulation for a ranged voltage analysis. Figure 5: Static analysis of displacement vs. Voltage for copper with a width of 0.048 μm This displacement is also shown in Figure 6 and Figure 7 as a function of time with pivot widths of 0.048 μm and 0.053 μm, respectively. The 0.053 μm thick pivot does not allow sufficient displacement due to its stiffness and prevents the contacts from closing.
  • 9. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME Figure 6: Dynamic analysis of displacement vs. Time using a copper pivot with a width of 0.048 μm Figure 7: Dynamic analysis of displacement vs. Time using a copper pivot with a width of 0.053 μm 81 Figure 8 also shows a graph of displacement of the beam as a function of time, using aluminium. Although aluminium has the same pivot thickness of 0.053 μm as the copper pivot shown in Figure 7, it provided a displacement which reached its target destination due to the innate flexibility of the material. Figure 8: Dynamic analysis of displacement vs. Time using an Aluminium pivot with a width of 0.053 μm
  • 10. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 82 A dynamic simulation was carried out using aluminium with a pivot thickness of 0.048 μm, however, the software reported that the aluminium pivot material exceeded its boundary conditions and failed, therefore no graph was produced. A separate experiment was conducted for the thickness of the pivot. Figures 9 and 10 show von mises stress and displacement vs the thickness of the aluminium and copper materials respectively, with a pulling voltage of 3 V. The experiments show aluminium to provide higher flexibility over copper at a thickness of 0.05μm, but compromises von mises stress that goes beyond its ultimate yield strength, which would lead to fracture failure. Copper provides an optimum displacement at the same thickness, with a von mises stress under the yield strength, which guarantees no deformity of the material during the electrostatic pulling force. Therefore, copper bulk general was selected as the pivot material, because of its intrinsic properties. Figure 9: Von Mises Stress and Displacement vs Thickness of Aluminium pivot at 3V Figure 10: Von Mises Stress and Displacement vs Thickness of Copper pivot at 3V
  • 11. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 83 8. CONCLUSION After numerous iterations of the design, the electrostatic supply voltage was reduced significantly from typical values exceeding 40 volts to 14 volts for copper bulk general. This was achieved using empirical analysis to observe each area of the structure for improvements. The maximum pulling force was achieved by making use of the surface area of the electrostatic plates on the beam and the base of the seesaw. Also, an improvement was made by optimising the thickness of the pivot to operate under von mises stress and applying the minimum voltage for increased reliability. A working simulation was achieved without compromising the ‘Air-Gap’ between the contacts, which retained isolation when the switch was open-circuited, with alternating pulses. By using dynamic analysis on Intellisuite software, the seesaw action was enabled. The seesaw RF MEMS switch is an improved concept over existing designs, which are limited to Single-Pole Single-Throw (SPST) switching [1] [4]. Additional contacts, in the improved design, achieve DPDT switching, and required lower actuation voltages, due to the reduction in size. The seesaw switch may be configured into three switching modes (SPST, SPDT and DPDT) making it a versatile component for use within integrated circuits for mobile communication devices. 9. ACKNOWLEDGMENT The authors’ acknowledgment is given to Jianhua Mao from Intellisense for his software support and valuable advice on Intellisuite modelling and simulation software tools. 10. REFERENCES [1] J. M CABRAL A.S. HOLMES, (2006). “A novel seesaw-type RF MEMS switch.” Electrotechnical Conference, 2006. MELECON 2006, IEEE Mediterranean 2006, pp. 288- 292. [2] K.HYOUK, C. DONG-JUNE, P.AE-HYOUNG, L. HEE-CHUL, P. YONG-HEE, K. YONG-DAE, N. HYO-JIN, J. YOUNG-CHANG B. JONG-UK (2007). “Contact materials and reliability for high power RF-MEMS switches.” Micro Electro Mechanical Systems, 2007. MEMS. IEEE 20th International Conference on 2007, pp. 231-234. [3] H. JAAFAR, N. FONG LI N.A.M. YUNUS (2011). “Design and simulation of high performance RF MEMS series switch.” Micro and Nanoelectronics (RSM), 2011 IEEE Regional Symposium on 2011, pp. 349-353. [4] K.JONGSEOK, K. SANGWOOK, Y. HONG, J. HEEMOON L. SANGHOON (2007). “Variable pivot seesaw actuated RF MEMS switch for reconfigurable system application.” Micro Electro Mechanical Systems, 2007. MEMS. IEEE 20th International Conference on 2007, pp. 775-778. [5] A.M. PASHA M.A. SAQIB (2009). “Design optimization for low voltage DC contact RF MEMS shunt switch.” Electrical Engineering, 2009. ICEE '09. Third International Conference on 2009, pp. 1-6. [6] H. R. Shea (2006), “Reliability of MEMS for space applications” Proc. of SPIE Reliability, Packaging, Testing, and Characterization of MEMS/MOEMS V on 2006, vol. Vol. 6111, 61110A. [7] J. HWANG, 2007. “Reliability of Electrostatically Actuated RF MEMS Switches” Radio- Frequency Integration Technology, 2007. RFIT 007. IEEE International Workshop on 2007, pp. 168-171.
  • 12. International Journal of Computer Engineering and Technology (IJCET), ISSN 0976-6367(Print), ISSN 0976 - 6375(Online), Volume 5, Issue 7, July (2014), pp. 73-84 © IAEME 84 [8] S. PRANONSATIT, G. HONG, A.S. HOLMES and S. LUCYSZYN, 2006. “Rotary RF MEMS Switch Based on the Wobble Motor Principle” Micro Electro Mechanical Systems, 2006. MEMS 2006 Istanbul. 19th IEEE International Conference on 2006, pp. 886-889. [9] Anesh K Sharma, Ashu K Gautam, CG Balaji, Asudeb Dutta and SG Singh, 2012. “Shunt Rf Mems Switch with Low Potential and Low Losson Quartz for Reconfigurable Circuit Applications”, International Journal of Electronics and Communication Engineering Technology (IJECET), Volume 3, Issue 2, pp. 497 - 510, ISSN Print: 0976- 6464, ISSN Online: 0976 –6472. 11. ABBREVIATIONS 2G Second Generation 3G Third Generation 4G Fourth Generation BIO MEMS Biological Micro Electro- Mechanical Systems DC Direct Current DPDT Double-Pole-Double-Throw GHz Giga-Hertz GPS Global Positioning System GSM Global System for Mobile Communications MEMS Micro Electro-Mechanical Systems MOMEMS Micro-Opto Electro- Mechanical Systems ms Milliseconds SPDT Single-Pole Double-Throw SPST Single-Pole Single-Throw SP8T Single-Pole Eight-Throw RX Receive RF MEMS Radio Frequency Micro Electro-Mechanical Systems TX Transmit μm Micrometre Wi-Fi Wireless Fidelity WiMAX Worldwide Interoperability for Microwave Access