Flow-induced instability of double-walled carbon nanotubes based on nonlocal elasticity theory

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Abstract

Instability occurs in double-walled carbon nanotubes when a fluid flows through them. This is investigated using an elastic shell model based on Donnell's shell theory. The dynamic governing equations of double-walled carbon nanotubes are derived on the basis of nonlocal elasticity theory, and the van der Waals interaction between the inner and outer walls is considered. Instability induced by a pressure-driven steady flow is studied. The numerical computations reveal that as the flow velocity increases, double-walled carbon nanotubes have a destabilizing style to get through multi-bifurcations of the first (pitchfork) and second (Hamiltonian Hopf) bifurcations in turn. It can be concluded that the critical flow velocity of the flow-induced instability is closely correlated to the ratio of the length to the radius of double-walled carbon nanotubes, the pressure of the fluid and the small size effects.

Highlights

► The critical flow velocity of the DWCNTs is correlated to the small size effects. ► The nonlocal natural frequencies of DWCNTs decrease as compared to local ones. ► As the flow velocity increases, DWNCTs get through multi-bifurcations in turn.

Introduction

Since the landmark paper by Iijima [1], carbon nanotubes (CNTs) have attracted worldwide attention due to their potential use in the fields of chemistry, physics, nano-engineering, electrical engineering and materials science. CNTs can be used as strong, light and high toughness fibers for composite structures, parts of nano-devices and for hydrogen storage [2], [3], [4], [5]. Although classical or local continuum models, such as beam and shell models, are practical in analyzing CNTs for large systems, however, size effects often become remarkable at nanometer scales, therefore, the modeling of size-dependent phenomena has become a topic of interest [6], [7]. Based on the theory of nonlocal elasticity [8], the scale effect was clarified in elasticity by assuming the stress to be a functional of the strain field at every point in the body. In this sense, the internal size scale could be considered simply as a material parameter in the constitutive equations. The application of nonlocal elasticity models in nanomaterials was proposed by Peddieson et al. [9]. They applied the nonlocal elasticity to formulate a nonlocal version of Euler–Bernoulli beam model, and concluded that nonlocal continuum mechanics could potentially play an important role in nanotechnology applications. Further applications of the nonlocal continuum mechanics have been utilized in investigating the mechanical behavior of CNTs. Sudak [10] investigated the infinitesimal column buckling of multi-walled carbon nanotubes (MWCNTs) combining not only van der Waals forces but also the effects of small length scales. His results demonstrated that as the small length scale gets larger in magnitude the critical axial strain gets smaller compared to the results with classical continuum mechanics. Zhang et al. [11] investigated a nonlocal multi-shell model for the axial buckling of MWCNTs under axial compression. Their results indicated that both the buckling mode and the length of tubes have contributions to the influence of the small scale on the axial buckling strain. Zhang et al. [12], [13] adopted the theory of nonlocal elasticity to investigate free transverse vibrations of double-walled carbon nanotubes. Wang and Hu [14] investigated flexural wave propagation in single-walled carbon nanotubes, their study focuses on the wave dispersion by considering a model of traditional Timoshenko beam in conjunction with the theory of nonlocal elasticity. Wang [15] studied wave propagation in carbon nanotubes by nonlocal continuum mechanics. They investigated wave propagation in CNTs with both Euler–Bernoulli and Timoshenko beam models by considering the nonlocal elasticity.

Recently, fluid flow inside CNTs has become an interesting subject. The properties of fluidity, diffusivity, and viscosity, and the dynamics of fluid in a fine pore have been investigated [16], [17]. The dynamic properties of hydrogen bonding [18], the effects of wall–fluid interaction [19], the dependence of fluid behavior on the spatial size of CNTs [20], and other issues have been extensively investigated in the nanoflow and microflow fields. The instability problems of fluid-filled CNTs are of central interest in the field. Wang et al. [21] investigated the elastic buckling of multi-walled carbon nanotubes (MWCNTs) under external radial pressure using a multi-walled shell model, and the results demonstrated that the multi-walled shell model is in good agreement with the experiment. Recently, the flow-induced instability of single-walled carbon nanotubes (SWCNTs) has been investigated by modeling carbon nanotubes with the Eulerian beam model [22]. Besides, Donnell's shell model for fluid-conveying MWCNTs with the consideration of the van der Waals interaction has been presented in Ref. [23]. Wang [24] developed a nonlocal double-elastic beam model to perform the vibration analysis of double-walled carbon nanotubes conveying fluid. Lee and Chang [25] investigated the vibrations of fluid-conveying double-walled carbon nanotubes by adopting a nonlocal double-elastic beam model. Wang [26] initiated a theoretical analysis of wave propagation of fluid-conveying single-walled carbon nanotubes based on strain gradient elasticity theory with consideration of both inertia and strain gradients, in which two small-scale parameters were accounted for. Wang [27] developed a new theoretical model, based on the modified couple stress theory, for the vibration analysis of fluid-conveying microtubes by introducing one internal material length scale parameter.

The purpose of the present paper is to investigate the small scale effects on the flow-induced instability of double-walled carbon nanotubes (DWCNTs) using Donnell's shell model.

Section snippets

Nonlocal elasticity theory

Based on Eringen nonlocal elasticity model [28], the stress at a reference point x in a body is considered as a function of strains of all the points in the near region. The above assumption is in agreement with the atomic theory of lattice dynamics and experimental observations on phonon dispersion.

Consider a homogeneous and isotropic elastic solid, the constitutive equation isσ(x)=C0:Vα(|xx|,τ)ε(x)dV(x),where symbols ‘:’ is the inner product with double contraction, C0 is the elastic

Small scale effect on coupled shell model for DWCNT conveying fluid

In Fig. 1, DWCNTs with van der Waals interaction between the inner and outer walls are modeled using Donnell's cylindrical shell theory [29]. The fluid inside the inner tube is assumed to be an ideal incompressible, and the flow is driven by pressure. The small scale effect is considered by using the nonlocal elasticity theory stated before.

The governing equations of motion of the model are written as follows [30]:D4w1+ρth2t2(1(e0a)22)w1=(1(e0a)22)(c12(w1w2))(1(e0a)22)p+1R12F1x2,D4

Numerical computations and discussions

Two quantitative comparisons are performed to prove the validity of the present approach. In quantitative comparisons, first of all, the numerical results based on the present study are compared with those obtained from Ref. [24]. All the input data must be exactly the same for comparison, therefore, the gap between the two walls is taken as h=0.34 nm, Young's modulus of the DWCNT is E=1 TPa, and the mass density is ρt=2300 kg/m3 for CNTs and pf=1000 kg/m3 for the fluid. The inner radius and outer

Conclusions

Fluid-conveying double-walled carbon nanotubes (DWCNTs) are modeled based on Donnell's shell theory by taking into account the van der Waals interaction between the inner and outer walls, in conjunction with the consideration of the small scale effects by nonlocal elasticity theory. The instability that is induced by a pressure-driven steady flow is studied. The numerical computations indicate that as the flow velocity increases, DWNCTs have a way to get through multi-bifurcations of the first

Acknowledgment

This research was partially supported by the National Science Council in Taiwan through Grant NSC-96-2221-E-327-018-MY2. The authors are grateful for this support.

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