-
1
-
-
45849156128
-
-
D. Fry, T. Sintes, A. Chakrabarti, and C.M. Sorensen, Phys. Rev. Lett. 89, 148301 (2002).10.1103/PhysRevLett.89.148301
-
(2002)
Phys. Rev. Lett.
, vol.89
, pp. 148301
-
-
Fry, D.1
Sintes, T.2
Chakrabarti, A.3
Sorensen, C.M.4
-
4
-
-
0038796921
-
-
A.E. González, Phys. Rev. Lett. 86, 1243 (2001).10.1103/PhysRevLett.86.1243
-
(2001)
Phys. Rev. Lett.
, vol.86
, pp. 1243
-
-
-
5
-
-
0034683239
-
-
J. Blum et al, Phys. Rev. Lett. 85, 2426 (2000).10.1103/PhysRevLett.85.2426
-
(2000)
Phys. Rev. Lett.
, vol.85
, pp. 2426
-
-
Blum, J.1
-
7
-
-
0000221350
-
-
C.F. Schmid and D.J. Klingenberg, Phys. Rev. Lett. 84, 290 (2000); 10.1103/PhysRevLett.84.290
-
(2000)
Phys. Rev. Lett.
, vol.84
, pp. 290
-
-
-
8
-
-
0034215437
-
-
C.F. Schmid, L.H. Switzer, and D.J. Klingenberg, J. Rheol.JORHD2 44, 781 (2000).10.1122/1.551116
-
(2000)
J. Rheol.
, vol.44
, pp. 781
-
-
-
9
-
-
85038289923
-
-
www.ts.nist.gov/ts/htdocs/230/232/232.htm
-
See C.R. Schultheisz, www.ts.nist.gov/ts/htdocs/230/232/232.htm SRM 2490 for instrument details.
-
-
-
Schultheisz, C.R.1
-
13
-
-
0036806473
-
-
E.K. Hobbie et al, J. Chem. Phys.JCPSA6 117, 6350 (2002).10.1063/1.1503769
-
(2002)
J. Chem. Phys.
, vol.117
, pp. 6350
-
-
Hobbie, E.K.1
-
14
-
-
0346505865
-
-
A.J. Bray, Adv. Phys. 43, 357 (1994). The binary field (Formula presented) has Ising symmetry and is not conserved.
-
(1994)
Adv. Phys.
, vol.43
, pp. 357
-
-
Bray, A.J.1
-
15
-
-
42749101558
-
-
L.E. Becker and M.J. Shelley, Phys. Rev. Lett. 87, 198301 (2001).10.1103/PhysRevLett.87.198301
-
(2001)
Phys. Rev. Lett.
, vol.87
, pp. 198301
-
-
-
17
-
-
0022076399
-
-
C.E. Chaffey and R.S. Porter, J. Rheol.JORHD2 29, 281 (1985).10.1122/1.549792
-
(1985)
J. Rheol.
, vol.29
, pp. 281
-
-
-
21
-
-
0034723247
-
-
M. F. Yu et al, [Science 287, 637 (2000)] measure the deformation of comparable MWNTs. The Young’s modulus (Formula presented) and bending stiffness (Formula presented) compare with 7.5�MPa and (Formula presented), respectively, for typical organic fibers
-
(2000)
Science
, vol.287
, pp. 637
-
-
Yu, M.F.1
-
22
-
-
0142007113
-
-
The toluene suspensions contain a succinimide polymer (Formula presented) MWNT by mass, PIB soluble) that acts as a dispersant via preferential wetting on the MWNT surface [C. Park et al, Nanotechnology 14, L11 (2003)]. These suspensions are only marginally stable, however, with weak flocculation occurring over the course of days, but gentle shaking redisperses the tubes, consistent with an attraction of order (Formula presented), and hydrodynamic forces dominate in the non-Brownian PIB suspensions of interest. The graphite-graphite coefficient of static friction (0.1) compares with 0.5 for typical organic fibers, but simulations suggest that attractive interactions lead to order-of-magnitude enhancement
-
(2003)
Nanotechnology
, vol.14
-
-
Park, C.1
-
23
-
-
0002672677
-
-
B. Herzhaft et al, Phys. Rev. Lett. 77, 290 (1996).10.1103/PhysRevLett.77.290
-
(1996)
Phys. Rev. Lett.
, vol.77
, pp. 290
-
-
Herzhaft, B.1
-
25
-
-
0042945999
-
-
F.H. Garner and A.H. Nissan, Nature (London) 158, 634 (1946)
-
(1946)
Nature (London)
, vol.158
, pp. 634
-
-
-
27
-
-
0000882509
-
-
E.K. Hobbie and K.B. Migler, Phys. Rev. Lett. 82, 5393 (1999).10.1103/PhysRevLett.82.5393
-
(1999)
Phys. Rev. Lett.
, vol.82
, pp. 5393
-
-
-
29
-
-
0242289588
-
-
S. Lin-Gibson et al, J. Chem. Phys.JCPSA6 119, 8080 (2003).10.1063/1.1609972
-
(2003)
J. Chem. Phys.
, vol.119
, pp. 8080
-
-
Lin-Gibson, S.1
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