Document Type : Research Paper
Author
Faculty of Mechanical Engineering, Urmia University of Technology, Urmia, Iran
Abstract
Keywords

Mechanics of Advanced Composite Structures 2 (2015) 5560


Semnan University 
Mechanics of Advanced Composite Structures journal homepage: http://macs.journals.semnan.ac.ir 
Adaptive Tunable Vibration Absorber Using Shape Memory Alloy
S. Faroughi^{*}
Faculty of Mechanical Engineering, Urmia University of Technology, Urmia, Iran
Paper INFO 

ABSTRACT 
Paper history: Received 19 October 2015 Received in revised form 9 November 2015 Accepted 18 November 2015 
This study presents a new approach to control the nonlinear dynamics of an adaptive absorber using shape memory alloy (SMA) element. Shape memory alloys are classified as smart materials that can remember their original shape after deformation. Stress and temperatureinduced phase transformations are two typical behaviors of shape memory alloys. Changing the stiffness associated with phase transformations causes these properties of SMA. A thermomechanical model (based on the transformation strain which is a measure of strain indicating the phase transformation) is used to constrain the general thermomechanical features of the SMA. Here, the onedimensional SMA model is adopted to calculate both the pseudoelastic response and the shape memory effects. The dynamic behavior of shape memory alloys is then investigated, and a Newmark method is adopted to analyze the nonlinear dynamic equations. Results demonstrate that the vibration of an initial system can be tuned using the SMA absorber in a wide range of frequencies. Therefore, SMAs as adaptive tuned vibration absorbers provide an excellent performance to control vibrations. 



Keywords: Shape memory alloy Vibration absorber Phase transformation Nonlinear dynamic 


© 2015 Published by Semnan University Press. All rights reserved. 
Shape memory alloys (SMAs) are smart materials possessing remarkable properties, e.g. the ability to remember their original shape that is restored after applying a thermal load. In these kinds of alloys, in fact, a temperature increase may cause the full recovery of residual strains following loadingunloading mechanical processes. This property emerges as a result of a phase shift by which the crystal structure is reorganized. This atomic rearrangement can also occur when a stress field is imposed: thermal and mechanical fields show a reciprocal influence, i.e. the action of one of the two fields amends the characteristic values of the other. Another main characteristic of these materials is their thermomechanical behavior. This particular behavior of SMAs is due to their natural capability to go through the stresstemperaturedependent and reversible phase transformations. Pseudoelasticity and shape memory effects are the two main macromechanical properties of SMAs that result in the reversible martensitic phase transformation. Shape recovery can occur in two distinct ways, (1) when the material is deformed at low temperature, its original shape can be recovered by heating it above a characteristic temperature, the socalled shape memory effect (SME), and (2) when the material is deformed at high temperature, its original shape can be recovered by simply removing the applied load, the socalled superelasticity or the pseudoelasticity effect (SE).
Vibration control is an essential task in different engineering applications. Active and passive procedures are two wellknown methods in order to reduce the vibration of systems. The tuned vibration absorber (TVA) is a wellfixed passive vibrationcontrolling device that can be employed to achieve a reduction in the vibration of a primary structure under a particular external excitation [1, 6]. Generally, a TVA composed of a secondary system is attached to the primary device to absorb the vibration energy from the primary device. Such a device has different forms; however it normally acts like a springmass system [3]. To reduce the vibration amplitude of the primary device using a TVA, the natural frequency of TVA is equated with the frequency of the external forcing. Note that the TVA is not useful for systems where the frequency of the external forces varies or may not be known a priori [5]. To remove this limitation, the contribution of an adaptive tuned vibration absorber (ATVA) is used. The ATVA device is similar to that of TVA; however, it has adaptive elements that are employed for a tuned condition [2]. The tuned condition is maintained using a variable stiffness element to adjust the natural frequency of the absorber during the entire operation time [4]. Shape memory alloys are favorable materials for this goal (stiffness variation) due to their thermomechanical coupling characteristics. The SMA devices are used in many engineering applications. SMAs are used to investigate adaptive dissipation due to the mechanical property and hysteresis loop [9, 10]. Sitnikova et al. [11] and Santos et al. [12] demonstrated that SMAs could be used for vibration reduction as it was shown that the high dissipation capacity of SMAs changed the system response. Saadat et al. [13] and Lagoudas [14] used SMAs in a number of approaches to passively control the vibration. Elahini et al. [8] showed that the unique SMA characteristics (mentioned above) encouraged the theory of an ATVA because of the stiffness variation. In other words, the SMA can lead to softening the elastic modulus of the material at lower temperature, and to its hardening at higher temperature. Savi et al. [15] conducted a numerical study of an adaptive vibration absorber, and showed that the SMA could be used for ATVA devices. Wang et al. [16] also investigated the nonlinear dynamics of SMAs in tuning structural vibration frequency.
This study presents the application of SMAs for ATVA devices. The key properties of SMAs, the pseudoelasticity and the shape memory by phase transformation are taken into account. Here, a threedimensional thermomechanical model for SMAs proposed by Souza [17] and modified by Auricchio and Petrini [18] is used. The reason behind this choice is that, in this model, only one single internal variable is used. In other words the SMA characteristics can be easily modeled by this model.
The study is outlined as follows; the constitutive model applied to explain the thermomechanical characteristics of the SMA is presented in section 2, Numerical examples are provided in section 3, and finally, in section 4, some conclusions are drawn.
This section describes the onedimensional thermomechanical model deduced from a 3D constitutive SMA model which is developed by Souza [17] and modified by Auricchio and Petrini [18]. In this model, the total strain,and the absolute temperature, are considered as the controlling variables. The transformation strain which is a measure of strain showing the phase transformation (conversion from austenite or multiplevariant martensite to the singlevariant martensite) is assumed to be an internal variable. A free energy function is defined as [17],
(1) 
where, E is the module of elasticity, and is the material parameter related to the slope in the stresstemperature relationship in the phase transformation. h symbolizes the hardening of the material during the phase transformation, is the absolute temperature, and is a temperature below which no martensite phase transformation occurs. and denote the positive part and the Euclidean norm of the argument, respectively. The norm of the transformation strain, , is defined between zero and a maximum value which is a material parameter associated with the maximum transformation strain achieved at the end of the transformation. The indicator function, , in Eq. (1) is defined as,
(2) 
The state laws can be obtained from the energy function, Eq. (1), that lead to [17,18],
(3) 
where X is the thermodynamic force associated with the transformation strain, and is defined by,
(4) 
A limit function F, which is in terms of the relative stress X, is described to control the evolution of the internal variable ,
(5) 
In Eq. (5), R shows the radius of the elastic domain. Here, a onedimensional rod element is used instead of spring element; and thus, the onedimensional model is supposed, so that and also . These assumptions are valid as the SMA devices are only subjected to axial loads, and the fact that the highest value of the transformation strain occurs in this direction. The phase transformation strain matrix for a 1D model takes the following form for the case of uniaxial phase transition in the SMA material,
(6) 
where is the only variable used to describe whether the phase transition occurs in the material. The Euclidean norm of the phase transformation tensor is determined . Following the 1D assumptions listed above, the state laws in Eq. (3) thus are reduced to,
(7) 
A Misestype yield function that depends only on the first component of the thermodynamic force tensor, :
(8) 
The Kuhn–Tucker applied conditions must be introduced as follows in order to complete the model:
(9a) 
where is the socalled plastic multiplier, and corresponds to the phase transition parameter by
(9b) 
The above equations, Eqs (9a) and (9b), are called the flow rule. Fig. 1 schematically shows the idea of employing a SMA oscillator as a vibration absorber. The oscillator is composed of a SMA rod, a linear viscous damper, c and an attached mass.
The oscillator is excited by a harmonic external force where and denote the amplitude and frequency of the external force, respectively. According to Newton’s second law, the equation of motion of the system reads
(10) 
where is the nonlinear restoring force provided by the SMA rod. The value of the nonlinear restoring force is calculated by , where the value of stress, , is determined using Eq. (7) at each time step, and parameter A denotes the crosssection area of the SMA rod. To numerically solve Eq. (10), the Newmark average acceleration method is used. Note that is a function of displacement. The discretization of Eq. (10) at time step n+1 gives
(11) 
where denotes the equivalent dynamic outofbalance forces. If all necessary information from the time step n is known, Eq. (10) can be solved using a predictorcorrector method.
The equivalent SMA nonlinear force vector at time step n+1, is described by Eq. (12).
(12) 
where, denotes the dynamic tangent matrix at n^{th }time step and is the equivalent SMA nonlinear force at n^{th} time step.
Figure1. The forced oscillation of a dynamical system with two linear and nonlinear absorbers
At this point, the Newmark average acceleration method is applied to update the displacement, velocity, and acceleration as [19],
(13) 

where, is the time step. Eq. (11) is again recalculated using the updated displacement, velocity and acceleration, as shown in Eq. (13). If the equivalent dynamic outofbalance forces are not zero, the NewtonRaphson corrector must be applied. After some algebraic work, the improvement can be obtained as
(14) 
where, is the dynamic tangent matrix which is identical to that of the predictor step. The iterative improvements for and are defined as,
(15) 
These procedures are repeated until the equivalent dynamic outofbalance force falls below a given value.
In the following section, numerical examples supporting the idea of implementing SMAs in the ATVA devices are explored.
To verify the nonlinear dynamical model of SMAs, results of the model presented in section 2 are compared to that of Savi et al. [15]. To this end, a system with one degree of freedom is considered as depicted in Fig.1. In the linear analysis, it is assumed that and where is the dimensionless natural frequency of the linear system and is the dimensionless frequency of the SMA system. The excitation frequency is considered as .
For the analysis, a NickelTitanium alloy with the physical specifications of and is considered. The reference temperature is assumed in the oscillatory SMA system. Two conditions are analyzed using and where shows damping ratio. Other thermomechanical characteristics of considered NiTi alloy are reported in Table 1.
The linear response of the system for and are shown respectively in Figs. 2 and 3.
Figs. 4 and 5 show the response of the SMA system with and . The obtained results are in a good agreement with the work of Savi et al. [15], however, the presented model has a higher convergence speed.
The results shown in Figs. 4 and 5 show that the response of the SMA system tends to present smaller vibration amplitudes when compared to those obtained by the elastic system. Consequently, it reduces vibrations to a higher extent indicating an increase in the energy dissipation with respect to that of using a linear elastic spring. Figures 4 and 5 also illustrate that the presented model has a satisfactory precision with one half required computational cost to the model of Savi et al. [15].
To further demonstrate the applicability of SMA elements and the robustness of the presented model, a system using SMA elements with two degrees of freedom is considered (see Fig. 6) where the effect of dynamic absorber is investigated.
As shown in Fig. 6, the initial system consists of a linear spring and a damper which are under the external force . The Secondary system includes a mass , spring and damper . The physical quantities of the constitunets of the system shown in Fig. 6 are considered as: , , and the external frequency .
Table 1. The assumed parameters for the shape memory alloy
244.05 
266.64 
221.45 
65 

0.33 
79 
5.4 

Figure 2. The linear system response for




Figure 3. Linear system response for 

Figure 4. The SMA system response for
Figure 5. The SMA system response for
Figure 6. A twodegree of freedom system excited under external force 
The following equations of motion for two DOF systems can be written as follows:
(16) 
In this example, the system is analyzed for under two operating temperatures and to show the effect of temperature. Fig. 7 illustrates the responses of the system to different temperatures. It is observed that the response of the initial system (i.e. the vibration amplitude) at is smaller than that of computed at . These results clearly highlight that changing the temperature can reduce the viberation amplitude of the system with respect to different frequencies. This behavior is due to the superelasticity property of the SMA.
This study discusses the use of SMA elements in the adaptive tuned vibration absorbers. Initially, a system with one degree of freedom oscillator is considered in which the restitution force is given by the SMA element. The results illustrate that the vibration response of the system has smaller amplitudes when the SMA element has higher energy dissipation rates. A system with two degrees of freedom is then investigated where SMA elements make the secondary system. Results from these analyses show that the SMA system response with dynamic absorber can be tuned within a specific frequency range. This shifts the initial natural frequency of the system away from the resonance.
This attenuation can be changed using the operating temperature related to the thermomechanical behavior of SMA elements. It should be noted that the presented model in this study has some advantages with regard to other models, e.g., the rate of convergance is increased by two times, and this has easily modeled the two typical behaviors of shape memory alloys.
Figure 7. The SMA system response at the temperatures of and
Reference
[1] Meirovitch L. Elements of Vibration Analysis. McGrawHill; 1986.
[2] Brennan MJ. Some Recent Developments in Adaptive Tuned Vibration Absorbers/Neutralisers. Shock Vib 2006; 13(4): 531–543, 2006.
[3] Rustighi E, Brennan MJ, Mace BR. A Shape Memory Alloy Adaptive Tuned Vibration Absorber: Design and Implementation. Smart Mater Struct 2005; 14: 19–28.
[4] Rustighi E, Brennan MJ, Mace BR., Realtime Control of A Shape Memory Alloy Adaptive Tuned Vibration Absorber, Smart Mater Struct 2005; 14(6) 1184–1195.
[5] Wang L, Melnik RVN. Nonlinear Dynamics of Shape Memory Alloy Oscillators in Tuning Structural Vibration Frequencies. Mechatronics 2012; 22(8): 1085–1096.
[6] Inman DJ. Vibration: with Control, Measurement and Stability. Prentice Hall; 1989.
[7] Lagoudas DC. Introduction to Modeling and Engineering Applications of Shape Memory Alloys. Springer; 2007.
[8] Elahinia MH, Koo JH, Tan H. Improving Robustness of Tuned Vibration Absorbers using Shape Memory Alloys. Shock Vib 2005; 12(5): 349–361.
[9] Van JH. Damping Capacity of Thermoelastic Martensite in Shape Memory Alloys. J Alloys Compd 2003; 355 (1–2): 58–64.
[10] Sitnikova E, Pavlovskaia E, Wiercigroch M. Dynamics of An Impact Oscillator with SMA Constraint, Eur Phys J Special Topics 2008; 165(1): 229–238.
[11] Sitnikova E, Pavlovskaia E, Wiercigroch M, Savi MA. Vibration Reduction of The Impact System by An SMA Restraint: Numerical Studies. Int J Nonlinear Mech 2010; 45(9): 837–849.
[12] Santos DD, Cardozo B, Savi MA. Nonlinear Dynamics of A Nonsmooth Shape Memory Alloy Oscillator. Chaos Solitons Fractals 2009; 40(1): 197–209.
[13] Saadat S, Salichs J, Noori M, Hou Z, Davoodi H, Baron I, Suzuki Y, Masuda A. An Overview of Vibration and Seismic Applications of NiTi Shape Memory Alloy. Smart Mater Struct 2002; 11(2): 218–229.
[14] Lagoudas DC, Machado LG, Lagoudas M. Nonlinear Vibration of A Onedegree of Freedom Shape Memory Alloy Oscillator: A NumericalExperimental Investigation. Proc AIAA Conf 2005.
[15] Savi M, Paula A, Lagoudas D. Numerical Investigation of An Adaptive Vibration Absorber Using Shape Memory Alloys. J Intell Mater Sys Struct 2011; 22(1): 67–80.
[16] Wang LX, Melnik RVN. Tuning Vibration Frequencies with Shape Memory Alloy Oscillators. Proc Int Conf Comput Struct Technol 2006.
[17] Souza AG, Mamiya EN, Zouain N. Threedimensional Model for Solids Undergoing Stressinduced Phase Transformations. Eur J Mech A Solids 1998; 17(5): 789–806.
[18] Auricchio F, Petrini L. Improvements and Algorithmical Considerations on A Recent Threedimensional Model Describing Stressinduced Solid Phase Transformations. Int J Numer Methods Eng 2002; 55(11): 1255–1284.
[19] Crisfield MA, Nonlinear Finite Element Analysis of Solids and Structures. John Wiley & Sons; 1997.