Compression behavior of carbon nanotube bundles and individual carbon nanotubes within the bundle has been studied by using the Suzuki, Shanker, and usual Tait formulations. It is found that the Suzuki formulation is not capable of explaining the compression behavior of nanomaterials. Shanker formulation slightly improves the results obtained by the Suzuki formulation, but only usual Tait’s equation (UTE) of state gives results in agreement to the experimental data. The present study reveals that the product of bulk modules and the coefficient of volume thermal expansion remain constant for carbon nanotubes. It has also been found that the individual carbon nanotubes are less compressible than bundles of carbon nanotubes.
1. Introduction
After their discovery by Iijima [1] carbon nanotubes have got a lot of attention because of their unique electronic and mechanical properties, but the most important property of carbon nanotubes is their elastic response to the external force or stress [2, 3]. As a one-dimensional structure, carbon nanotubes can be thought of as one sheet or multiple sheets of graphene rolled into a cylinder. Single-walled carbon nanotube bundles typically consist of several nested tubes, each like a graphene sheet bent into the cylindrical form with an overall diameter of a few nanometers. According to different chiral angles, single-walled carbon nanotubes can be classified into zigzag (θ=0°), armchair (θ=30°), and chiral tubes (0°<θ<30°) [4]. The Young’s modulus and Poisson’s ratio of nanotube have been studied by the previous workers [5–9], while the hardness as one of the most important parameters characterizing the mechanical properties of single-walled carbon nanotubes has been intensively studied during the last decade [6, 10].
High pressures which are encountered from deep down the earth to the astrophysical objects may cause many effects such as compression, pressure ionization, modification in electronic properties, phase changes, and several phenomenons in applied fields [11]. For this, pressure versus volume relations of condensed matter known as equation of state is a vital input. Many equations of state exist in the literature, but still there is a need to judge on their suitability under whole range of compressions as most of them give the same result under small compression.
In high pressure, generally used theory is the finite strain theory which means the theory due to Birch [12]. However, Birch’s theory rates no more than a passing mention as discussed in detail by Stacy [13]. The attention has also been given to the theory based on atomic potential as presented by Rydberge [14]. The Mie Grüneisen theory was followed by Suzuki et al. [15, 16] and reported what became known as Suzuki formulation [16–18]. The Grüneisen theory of thermal expansion as formulated by Born and Huang [19] has been used by Shanker et al. [20]. These authors included a higher order term for the change in the expansion of potential energy. Using some thermodynamical relation Tait formulated a relation [21–23] known as UTE.
In the present work, we have investigated the mechanical properties especially volume compression (V/V0) of nanotube bundles and individual carbon nanotubes using widely used Suzuki, Shanker, and usual Tait equation of state (EOS) [15–23]. We have then compared our calculated results with the experimental values as well as with the results obtained for graphite. For input parameters the values of bulk modulus and its first order pressure derivative of nanotube bundle (K0 = 37 GPa, K01 = 11) and individual tube within the bundle (K0 = 230 GPa, K01 = 4.5) have been taken from the work of Reich et al. [24] who have used local-density approximation of density-functional theory to calculate these values. For graphite the values of bulk modulus and its first order pressure derivative are taken to be K0 = 33.8 GPa and K01 = 8.9, as measured by Hanfland et al. [25] from X-ray diffraction studies.
2. Method of Analysis
Based on Mie-Grüneisen Debye theory Suzuki et al. [15, 16] have derived an EOS, known as the Suzuki equation [18, 26], to study the change in volume V/V0 with temperature T, along an isobar. This Suzuki equation has been widely used in the literature [15–18], and its mathematical form reads as follows [27]:
(1)VV0=[1+2k-(1-4kETh/Q)]1/22k,
where k=(K0′-1)/2, ETh is the thermal energy, Q=K0V0/γ0, and γ0 is the Grüneisen ratio. K0, K0′ are the isothermal bulk modulus and its first order pressure derivative, respectively. The subscript o refers to their value at P=0 and T=300 K. Using the well known relation [27] γ0ETh/V0 = PTh, (1) reads as follows [28]:
(2)VV0-1=1-[1-2((K0′-1)/K0)PTh]1/2K0′-1,
where PTh is the thermal pressure.
Shanker et al. [20] have argued that if P is not equal to zero, (2) may be rewritten as follows:
(3)VV0-1=1-[1-2((K0′-1)/K0)(PTh-P)]1/2K0′-1.
Now, when thermal pressure is zero (PTh=0), (3) gives the following simple relation:
(4)VV0-1=1-[1+2((K0′-1)/K0)P]1/2K0′-1.
This is Suzuki EOS.
Shanker et al. [20] have reported an isobaric EOS, using the Grüneisen theory of thermal expansion as formulated by Born and Huang [19] whose mathematical form reads as follows:
(5)VV0-1=1-[1-2((K0′+1)/K0)PTh]1/2K0′+1.
It has been argued by Shanker et al. [20] that when P is not equal to zero, (5) may be rewritten as follows:
(6)VV0-1=1-[1-2((K0′-1)/K0)(PTh-P)]1/2K0′-1.
When thermal pressure is zero (PTh=0), (6) gives
(7)VV0-1=1-[1+2((K0′+1)/K0)P]1/2K0′+1.
This is Shanker EOS.
The usual Tait equation of state is obtained by assuming the fact that the product of the thermal expansion coefficient (α) and the bulk modulus (KT) is constant under the effect of pressure [29], that is,
(8)αK=constant.
Differentiation of (8) with respect to volume at constant temperature gives
(9)α(dKdV)T+K(dαdV)T=0.
Anderson-Grüneisen parameter is defined as
(10)δT=Vα(dαdV)T,
where δT is Anderson-Grüneisen parameter at constant temperature.
From (9) and (10), we get
(11)δT=Vα(dαdV)T=-VK(dKdV)T.
Assuming δT to be independent of V,
(12)δT=(dKdP)T=K01.
Anderson-Grüneisen parameter δT and η=V/V0 are related by the following relation [28]:
(13)(δT+1)η=A,
where A is a constant for a given solid.
In view of (13), (11) can be written as
(14)dKK=[-AV0+1V]dV.
Integrating the previous equation, we get
(15)KK0=VV0expA[1-VV0],
where
(16)K=-V(dPdV)T.
In view of (16), (15) is written as
(17)KK0expA[1-VV0]dV=-dP.
The integration of (17) gives
(18)P=K0A[expA(1-VV0)-1].
Here, K0 is the bulk modulus at the zero pressure, and the constant A is determined from the initial conditions, namely, at V=V0, A=δT0+1.
Substituting the value of A in (18) and taking the natural log, we get the following final form of usual Tait equation of state:
(19)VV0-1=-ln[1+((K01+1)/K0)P]K01+1,
here the approximation δT0≈K01 is used.
To test the validity of this usual Tait’s equation of state we have employed it to predict the high pressure compression behavior of carbon nanotubes and graphite along with the Suzuki and Shanker EOSs.
Within the framework of UTE, the expression for the isothermal bulk modulus can be written as [30, 31]
(20)KTK0=VV0{1+K01+1K0P}.
3. Results and Discussion
Present analysis is based on the three widely used formulations, namely, Suzuki, Shanker, and usual Tait EOSs. We have calculated the values of compression (V/V0) at different pressures by using (4), (7), and (19) for individual CNT as well as nanotube bundles. Table 1 shows the variation of (V/V0) with pressure for individual as well as nanotube bundles. In Table 2, we have reported the values of the compression for graphite which may be treated as a bulk material. Thus we have analyzed the validity of equation of state for nanomaterials as well as bulk materials. For high pressure compression behavior, a graphical presentation between the calculated and experimental values has been shown in Figures 1 and 2. From tables and figures, it is clear that the results obtained by Suzuki formulation do not agree with the experimental data [24, 25] while Shanker formulation improves the results slightly. Moreover, it seems that at low compressions all equation give the similar results. On the other hand usual Tait EOS (19) gives the results which are in close agreement to the experimental data [24, 25] for the entire range of pressure. For usual Tait EOS the agreement between the theoretically calculated and experimental values demonstrates that the product of bulk modules and the coefficient of volume thermal expansion remain constant for carbon nanotubes. While the failure of Suzuki and Shanker formulation may be attributed to the fact that their analysis is based on approximation. The Suzuki model is based on the Taylor series expansion of potential energy, and during this expansion higher order terms beyond second order have been neglected. This approximation must introduce serious errors as discussed in detail by Wang and Reeber [26]. Inspired with the Suzuki model, Shanker et al. [20] have also neglected higher order terms in deriving (7).
Volume compression with pressure for carbon nanotube bundles and individual carbon-nanotubes using different EOSs.
P (GPa)
V/V0(19)bundle
V/V0(7)bundle
V/V0(4)bundle
V/V0 (Exp [24])bundle
V/V0(19)individ.
V/V0(7)individ.
V/V0(4)individ.
V/V0 (Ex [24])individ.
1.0
0.9766
0.9763
0.9759
0.9769
0.9957
0.9957
0.9957
0.9944
1.5
0.9670
0.9663
0.9654
0.9638
0.9936
0.9936
0.9936
0.9925
2.0
0.9583
0.9570
0.9557
0.9513
0.9915
0.9915
0.9914
0.9900
2.5
0.9505
0.9484
0.9467
0.9425
0.9894
0.9894
0.9893
0.9888
3.0
0.9434
0.9403
0.9381
0.9400
0.9874
0.9874
0.9872
0.9863
3.5
0.9368
0.9326
0.9299
0.9350
0.9854
0.9854
0.9852
0.9838
4.0
0.9307
0.9253
0.9222
0.9238
0.9834
0.9834
0.9831
0.9825
4.5
0.9250
0.9184
0.9147
0.9213
0.9814
0.9814
0.9811
0.9800
5.0
0.9197
0.9117
0.9076
0.9188
0.9795
0.9794
0.9790
0.9781
5.5
0.9147
0.9052
0.9007
0.9088
0.9776
0.9775
0.9770
0.9776
6.0
0.9100
0.8990
0.8940
0.9063
0.9756
0.9754
0.9750
0.9757
6.5
0.9055
0.8930
0.8875
0.8981
0.9737
0.9736
0.9730
0.9738
7.0
0.9013
0.8872
0.8813
0.8963
0.9719
0.9718
0.9710
0.9720
7.5
0.8972
0.8815
0.8752
0.8900
0.9700
0.9699
0.9691
0.9702
8.0
0.8934
0.8760
0.8693
0.8875
0.9682
0.9680
0.9671
0.9683
Volume compression with pressure for graphite.
P (GPa)
V/V0 (Exp [25])
V/V0 (19)
V/V0 (7)
V/V0 (4)
0
1
1
1
1
2.0870
0.9618
0.9518
0.9504
0.9487
3.0434
0.9507
0.9356
0.9325
0.9296
4.8696
0.9204
0.9105
0.9027
0.8975
6.9565
0.8961
0.8878
0.8735
0.8656
8.3478
0.8809
0.8751
0.8559
0.8463
9.0434
0.8737
0.8693
0.8475
0.8372
10.434
0.8665
0.8586
0.8316
0.8197
11.913
0.8566
0.8483
0.8157
0.8022
13.913
0.8500
0.8359
0.7955
0.7798
Variation of relative compression (V/V0) with pressure for nanotube bundle.
Variation of relative compression (V/V0) with pressure for graphite.
In the present study from Tables 1 and 2 it is found that the graphite is more compressible than the nanotube bundle which is formed by rolling graphene sheets. We further extended usual Tait’s EOS to calculate bulk modulus and the variation of isothermal bulk modulus (KT) with pressure for nanotube bundle and individual tube within the bundle which are shown in Figures 3 and 4, while calculated values are given in Table 3. From Figures 3 and 4, it is clear that the isothermal bulk modulus increases with pressure and the compression decreases with pressure in these nanotubes and thus follows the same trend as in the bulk solids. The variation of bulk modulus with pressure could not be compared with the experimental values, as to the best of our knowledge the experimental data about the pressure dependence of bulk modulus for carbon nanotubes is not available in the literature. However, in future our calculated values may stimulate some experimental investigations regarding high pressure behavior of bulk modulus for carbon nanotubes.
Variation of bulk modulus with pressure.
P (GPa)
KT bundle
KT individual
1
47.853
234.487
1.5
53.183
236.725
2
58.459
238.952
2.5
63.685
241.166
3
68.866
243.394
3.5
74.007
245.611
4
79.109
247.817
4.5
84.176
250.012
5
89.209
252.221
5.5
94.212
254.394
6.0
99.186
256.583
6.5
104.132
258.761
7
109.053
260.955
7.5
113.948
263.112
8
118.820
265.287
Variation of isothermal bulk modulus (BT) with pressure for nanotube bundle.
Variation of isothermal bulk modulus (BT) with pressure for individual tube.
4. Conclusions
On the basis of overall descriptions, it may thus be concluded that the Suzuki formulation fails to explain the high pressure compression behavior of carbon nanotubes Shanker formulation improves the result of Suzuki formulation, but among the three formulations, the usual Tait EOS is more suitable to explain the elastic properties of nanomaterials. The reason for its success lies in the fact that the product of bulk modules and the coefficient of volume thermal expansion remain constant for carbon nanotubes.
IijimaS.Helical microtubules of graphitic carbonDresselhausM. S.DresselhausG.EklundP. C.VigoloB.PenicaudA.CoulonC.SauderC.PaillerR.JournetC.BernierP.PoulinP.Macroscopic fibers and ribbons of oriented carbon nanotubesDresselhausM. S.DresselhausG.SaitoR.Physics of carbon nanotubesLuJ. P.Elastic properties of single and multilayered nanotubesLuJ. P.Elastic properties of carbon nanotubes and nanoropesHernandezE.GozeC.RubioA.Elastic properties of single-wall nanotubesSánchez-PortalD.ArtachoE.SolerJ. M.RubioA.OrdejónP.Ab initio structural, elastic, and vibrational properties of carbon nanotubesvan LierG.van AlsenoyC.van DorenV.GeerlingsP.Ab initio study of the elastic properties of single-walled carbon nanotubes and grapheneYakobsonB. I.BrabecC. J.BernholcJ.Nanomechanics of carbon tubes: instabilities beyond linear responseSchillingJ. S.The use of high pressure in basic and materials scienceBirchF.Elasticity and constitution of the Earth's interiorStacyF. D.Finite strain, thermodynamics and the earth’s coreRydbergeR.Graphical representation of results of band spectroscopySuzukiI.Thermal expansion of periclase and olivine, and their anharmonic propertiesSuzukiI.OkajimaS.SeyaK.Thermal expansion of single-crystal manganositeAndersonO. L.HelfrichG.Practical use of Suzuki's thermal expansivity formulationBornM.HuangK.ShankerJ.KushwahS. S.KumarP.Theory of thermal expansivity and bulk modulus for MgO and other minerals at high temperaturesTaravilloM.BaonzaV. G.RubioJ. E. F.NúezJ.CáceresM.The temperature dependence of the equation of state at high pressures revisited: a universal model for solidsSinghM.SinghP. P.GuptaB. R. K.KumarM.Temperature and pressure dependence of elastic constantsKandpalD.SinghK. Y.GuptaB. R. K.On pressure dependence of the relative compression (V/V0) at room temperature for the solids : copper and lead as prototypesReichS.ThomsenC.OrdejonP.Elastic properties of carbon nanotubes under hydrostatic pressureHanflandM.BeisterH.SyassenK.Graphite under pressure: equation of state and first-order Raman modesWangK.ReeberR. R.The role of defects on thermophysical properties: thermal expansion of V, Nb, Ta, Mo and WKumarM.A comparative study of Suzuki and Kumar formulations for thermal expansivityAndersonO. L.IsaakD. G.OdaH.High-temperature elastic constant data on minerals relevant to geophysicsShankerJ.KumarM.Thermodynamic approximations in high-pressure and high-temperature physics of solidsSchlosserH.FerranteJ.VinetP.Pressure dependence of the melting temperature of metalsMacDonaldJ. R.Some simple isothermal equations of state